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Hindawi Publishing CorporationInternational Journal of Biomedical ImagingVolume 2013 Article ID 892152 12 pageshttpdxdoiorg1011552013892152
Research ArticleComparison of User-Directed and Automatic Mapping of thePlanned Isocenter to Treatment Space for Prostate IGRT
Zijie Xu1 Ronald Chen1 Andrew Wang1 Andrea Kress1 Mark Foskey12 An Qin3
Timothy Cullip1 Gregg Tracton1 Sha Chang1 Joel Tepper3 Di Yan3 and Edward Chaney12
1 Department of Radiation Oncology CB 7512 University of North Carolina Chapel Hill NC 27599 7512 USA2Morphormics Inc 240 Leigh Farm Road Durham NC 27707 USA3Department of Radiation Oncology William Beaumont Hospital Royal Oak MI USA
Correspondence should be addressed to Edward Chaney chaneymeduncedu
Received 11 March 2013 Revised 6 September 2013 Accepted 16 September 2013
Academic Editor Xishi Huang
Copyright copy 2013 Zijie Xu et al This is an open access article distributed under the Creative Commons Attribution License whichpermits unrestricted use distribution and reproduction in any medium provided the original work is properly cited
Image-guided radiotherapy (IGRT) adaptive radiotherapy (ART) and online reoptimization rely on accurate mapping of theradiation beam isocenter(s) from planning to treatment spaceThismapping involves rigid andor nonrigid registration of planning(pCT) and intratreatment (tCT) CT images The purpose of this study was to retrospectively compare a fully automatic approachincluding a non-rigid step against a user-directed rigid method implemented in a clinical IGRT protocol for prostate cancerIsocenters resulting from automatic and clinical mappings were compared to reference isocenters carefully determined in eachtCT Comparison was based on displacements from the reference isocenters and prostate dose-volume histograms (DVHs) Tenpatients with a total of 243 tCTs were investigated Fully automatic registration was found to be as accurate as the clinical protocolbut more precise for all patientsThe average of the unsigned 119909 119910 and 119911 offsets and the standard deviations (120590) of the signed offsetscomputed over all images were (avg plusmn 120590 (mm)) 11 plusmn 14 18 plusmn 23 25 plusmn 35 for the clinical protocol and 06 plusmn 08 11 plusmn 15 and 11plusmn 14 for the automatic method No failures or outliers from automatic mapping were observed while 8 outliers occurred for theclinical protocol
1 Introduction
Image-guided radiotherapy (IGRT) [1] off-line adaptive ra-diotherapy (ART) [2] and online reoptimization [3] involvepretreatment imaging taken here to be CT imaging A proce-dure held in common by all three methods is registration ofthe planning (pCT) and treatment (tCT) images to map theplanned isocenter to treatment space Accuracy and precisionof this step are important for delivering an accumulated dosedistribution that closelymatches the treatment planMappingmethods involve at least rigid registration Ideally a nonrigidstep would be included to account for differences in organshape between planning and treatment times (Figure 1) Thecomposite of the rigid and possibly nonrigidmatrices is thenused to map the planned isocenter to the tCT
Quantitative evaluation of isocenter mapping methods ismuddled by the lack of gold standards [4] In the absence of
standards this work retrospectively compared a fully auto-matic method against a user-assisted procedure used in aclinical protocol for IGRT for prostate cancer The studyfocused on tCTs from a conventional diagnostic scanner dueto the availability of clinical data However the approachapplies to kilovoltage cone-beam CT (CBCT) images asillustrated later
2 Methods
21 Clinical Protocol The clinical protocol (Table 1) waspracticed over the period 2005ndash2008 at the University ofNorthCarolina (UNC) as part of the routineworkflowduringevaluation of a CT-on-rails system [5] (Primatom SiemensMedical Solutions Concord CA)ThePrimatom system con-sists of a conventional CT scanner a set of rails between the
2 International Journal of Biomedical Imaging
Planned isocenter
(a)
Rigidly mapped isocenter
Nonrigidlymappedisocenter
(b)
Figure 1 (a) Axial slice from the pCT showing planning prostate (white) and isocenter (black) (b) Corresponding slice from the tCTshowing the prostate (black) segmented by automatic nonrigid model deformation The rigidly mapped isocenter comes from translatingthe planning prostate (dim white) to the tCT The nonrigidly mapped isocenter comes from applying the deformation matrix resulting fromautosegmentation to the planned isocenter
Table 1 Isocenter Mapping Methods
Clinical mapping Automatic mapping
1CT simulate Align patient with laser beams intersecting atsimulated isocenter Tattoo skin at centers of lateral and anteriorlaser beams
Import pCT structure sets and isocenter to MxAnatomy Fitmodels to planning contours
2 Plan Place crosshairs at planned isocenter in axial slice Markskin contour at lateral and anterior intersections with crosshairs Acquire tCT using standard procedures
3Prepare patient for treatment imaging Tape BBs to anterior andlateral skin tattoos Acquire tCT with laser beams centered onBBs
Import tCT Rigidly register pCT with pCT using automaticmultiscale procedure
4 Import tCT to PLanUNC Autoregister imaged BBs in tCT withskin marks in pCT from Step 2 Autosegment prostate in tCT
5Inspect registration by comparing prostate contours in pCTwith intensity patterns in the tCT Manually edit registration toget best match between contours and tCT intensities
Determine correspondences between pCT and tCT prostatemodels
6 Convert manual 119909 119910 119911 edits from Step 5 to table shifts relativeto laser beams Apply shifts gt3mm and treat
Map isocenter label from pCT to tCT via correspondence fromStep 5 (2)
scanner and the linac and a dual-purpose imagingtreatmentcouch that moves along the rails Patients under the IGRTprotocol were imaged before treatment and the couch wasrolled from the CT scanner into the image-guided treat-ment position The fixed geometry between the scanner andlinac allows cross calibration of the patient laser alignmentsystems and the rails facilitate moving the couch from thescanner into treatment position with minimal time delay ormechanical disturbance of patient geometry
All patients underwent simulation using a PhilipsAcQSim CT system [6] (Philips Healthcare Andover MA)The planning isocenter was localized during simulation andthe anterior and lateral laser crosshairs were tattooed accord-ing to standard practice Treatment planning and calculationof hypothetically delivered dose were accomplished withPlanUNC [7 8] (PLanUNC is a set of modular software toolsfor external beam treatment planning and dose calculation
development at UNC) During planning the dosimetristplaced the computer crosshairs at the planned isocenter andthen marked reference points in the pCT at the intersectionsof the computer crosshairs with the skin (Figure 2) Thesereference points defined the geometrically correct positionsof the anterior and lateral laser crosshairs based on patientgeometry at planning time Before acquisition of each tCTthe patient was positioned by aligning the tattoos on thepatientrsquos skin with the CT laser crosshairs After alignmentsteel BBs were taped to the skin at the center of eachlaserrsquos crosshairs (AP RampL lat) Assuming accurate lasercalibration this placement allows the treatment isocenter forthe initial patient position to be inferred from the imagedBBs Immediately after imaging the tCT was imported to theplanning system and the physicist defined the BB centers viapoint and click on a computer display screen The planningsystem then automatically registered the tCT and pCT by
International Journal of Biomedical Imaging 3
Planned isocenter
Ideal (marked)locations of BBs
(a)
Mapped isocenter
Imaged BBs
(b)
Figure 2 (a) Axial slice from the pCT showing planned isocenter inside the prostate (white contour) and the marked locations of BBs (b)Corresponding slice from the tCT showing the autosegmented prostate (black) nonrigidly mapped isocenter and imaged BBs
matching the BBs in the tCT with the ideal locations markedin the pCT The algorithm minimized sum(distance betweencorresponding points)2 The final step was interactive rigidregistration of the prostate ROIs using the planning contoursfor reference Table tilt around the lateral axis and rotationaround the craniocaudal axis were not allowed in the finaltwo steps because rotational errors were not handled duringpatient setup Since the prostate was not contoured in thetCT the final step relied on human judgment to match thepCT intensities and contours with the tCT intensity patternsin the prostate ROI Table displacements were computed bycomparing the coordinates of the mapped isocenter after BBregistration with the coordinates after interactive prostate-based registrationThe displacements were used to repositionthe treatment table Assuming accurate registration andrepositioning and no changes in patient anatomy betweentCT imaging and treatment times this procedure registeredthe mapped planned isocenter with the treatment isocenterIn typical practice of IGRT displacements are implementedonly when they exceed a predefined threshold In theUNC protocol the threshold was 3mm along a given axisHowever for comparison purposes this study assumed thatthe displacements were applied without error regardless ofmagnitude
22 Automatic MappingMethod Automapping (Table 1) wasperformed using a beta version of ARTSuite (MorphormicsInc Chapel Hill NC) installed at UNC (Effective July 162012 Morphormics Inc became a wholly owned subsidiaryof Accuray Inc Sunnyvale CA) ARTSuite is a DICOM-RTcompliant software system developed to support IGRT ARTand online reoptimization with tools for autosegmentationof pCTs and tCTs nonrigid mapping between treatment andplanning spaces and dose accumulation and analysis
Automapping (Figure 3) involved three major steps (1)multiscale rigid registration of the previously segmented pCTto the tCT (2)model-based autosegmentation of the prostatein the tCT [9 10] and (3) nonrigid mapping of the planningisocenter to the tCT using a transformation that includedthe rigid registration matrix and a nonstatistical nonrigiddiffeomorphism determined from correspondences betweenthe pCT and tCT prostate models
23 Patient Data Ten patients with a total of 243 tCTswere investigated All pCTs were acquired with contrast inthe bladder and one patient had contrast in the bladder andrectumThe pixel dimensions in the axial plane were 1mm times1mm and the slice thickness was 3mm for pCTs and tCTs
All patients were treatedwith step-and-shoot IMRTusingan anterior and six oblique fields to sim75Gy prescribed to apoint or isodose curve Treatment typically included a booststarting sim50Gy to reach the final dose Margins of 5mmand 3mm were applied to the planning target volume for theinitial and boost plans respectively
231 Model Fitting to Prostate Contours This study assumedthat the manually drawn prostate contours in the pCT weretrue at treatment time To facilitate model-based segmen-tation of the tCTs as described below a prostate modelwas fit to each set of planning contours using an approachbased on prostate shape statistics described by Merck et al[11] This process yielded a custom prostate atlas for eachpatient that was used during registration and segmentationof tCTs Contours were represented as many short linesegments joined together This representation caused smalldifferences between a contour and a model at sharp verticeswhere two line segments joined These differences wereless than 02mm per contour on average and were causedby smoothness constraints that forced the model to havecontinuous curvature
232Multiscale Rigid Registration Theoverall rigid registra-tion approach has similarities with that of Court and Dong[12] and Smitsmans et al [13] discussed later in Section 3 Tominimize compute time registration progresses from coarseto fine scale in three steps The output of each step serves as aprior for the following step Step (1) aligns the skin boundingboxes and registers the images by sliding the image data inthe bounding box in the pCT along the box for the tCT Theregistration algorithm computes the voxel count per slice in apredefined intensity window and aligns the images by findingthe best match between graphs of voxel count versus sliceposition for each image pair A bone window performs bestbut can fail when a ldquobrightrdquo contrast medium is used for thepCT In such cases Step (1) is ignored and the algorithm starts
4 International Journal of Biomedical Imaging
(a) (b)
(c) (d)
(e) (f)
Figure 3 Multiscale registration of a pCT with a CBCT The planning prostate segmentation is white ((a) (b)) Blended axial and sagittalslices of unregistered images ((c) (d)) Axial and sagittal slices of images registered via Step (1) ((e) (f)) Axial and sagittal slices of imagesregistered via mutual information in the prostate ROI (Step (3)) In this example there is little difference between the second and third steps
over at Step (2) which optimizes global mutual information(MI) using a gradient descent approach [14] To avoid con-vergence to a distant optimum the algorithm is run multipletimes with different starting points The result with the bestscore over all runs is selected as the output Step (3) is similar
to Step (2) but with MI computed over an ROI defined by theatlas prostate model As in the clinical procedure rotationsduring automatic registration were not allowed explicitlyHowever the segmentation step treated rotation as a nonrigiddeformation in images with adequate intensity information
International Journal of Biomedical Imaging 5
Rigidly registered prostate model
Deformedprostatemodel
Gas bubble
Bone overlap
Figure 4 Midsagittal slice from a tCT illustrating how prostaterotation is treated as a deformation The white outline is the atlasprostate after automatic registration to the tCTThe black dashes arethe deformed atlas in the tCT
In Figure 4 for example the rigidly registered prostatemodeloverlaps pubic bone anteriorly causing the model to deformin a manner that avoids overlap with both the bone and thegas bubble in the rectum
233 Model-Based Autosegmentation The model used torepresent the prostate consists of a chain of so-called medialatoms (Figure 5) A full collection of atoms for an organis called a medial-representation (m-rep) [9] The chainconfiguration is well suited for objects that are more or lesstube-like including objects with closed ends Each prostateatom has a hub and 16 spokes radiating to the organsurface Additional hubs and spokes can be interpolated asneeded The skeletal framework serves as an organ-relativecoordinate system with a formalism for converting backand forth between model and image coordinates [9 15]After deformation of the starting model in a target imagecorresponding positions are defined by pairing points in thestarting and deformed models that have the same model-relative coordinates (Figure 5) The nonrigid transformationmatrix can be specified in image coordinates in terms of astandard displacement vector field [16] where each vectororiginates on a voxel in the reference image and terminates onits postdeformation position in the target image In contrastto voxel-scale deformations the model approach is statisticalat the scale of an organ but nonstatistical at voxel scaleeliminating small-scale artifacts [16]
Segmentation of the prostate in the tCT is necessaryto determine corresponding points in the pCT and tCTThe algorithm transfers the atlas model to the tCT usingthe rigid registration matrix and autosegmentation proceedsin a statistical framework based on Bayesrsquo theorem [9] Aconjugate gradient algorithm seeks to find the optimal model119872opt such that
119872opt = argmax119872isin119904
[log119901 (119872) + log119901 (119868 | 119872)] (1)
where 119872 is the currently deformed model in the trainedshape space 119904 [11] 119868 is the target image intensity patternrelative to 119872 119901(119872) is the probability of 119872 (geometrictypicality) and 119901(119868 |119872) is the probability of 119868 given119872 (imagematch [17])
234 Mapping the Isocenter The rationale for using a modelto map the isocenter stems from several considerations (1)during planning the isocenter is positioned relative to theprostate (2) a point in an image can be more accuratelyfoundby relying on regional image features that are correlatedspatially with the point rather than using local informationnear the point itself [18] and (3) the trainable models usedin this study provide a means for determining both the rigidand nonrigid components of the mapping transformationThe mapping step is straightforward and involves labelingthe point in the tCT that has the same prostate-relativecoordinates as the planned isocenter using (2)
VAL1015840Mapped (1198721015840(1198941015840 1198951015840 1198961015840)) = VAL (119872 (119894 119895 119896)) (2)
where 119872 1198721015840 = prostate models in pCT and tCT respec-tively 119894 119895 119896 and 1198941015840 1198951015840 1198961015840 are corresponding positions in119872- and 1198721015840-relative coordinates VAL = value of scalar forexample label dose or intensity in the pCT at 119872-relativeposition 119894 119895 119896 and VAL1015840Mapped = value of scalar mapped to1198721015840-relative position 1198941015840 1198951015840 1198961015840
24 Reference tCT Isocenters The clinical and automappingprotocols yielded two independent sets of tCT isocentersTo compare these sets a reference isocenter was determinedfor each tCT by repeating the automapping procedure withhuman supervision The main task was to reposition andoredit the autosegmented prostate as necessary to achieve thebest match with the tCT image data while generally preserv-ing the global shape and volume defined by the planningcontours Every rigid registration and prostate segmentationwere evaluated and edited based on human judgment afterwhich the tCT isocenter from (2) was accepted withoutmodification This procedure was performed without thepressure of clinical time constraints over sim8 months by twophysicists and a dosimetrist working as a team In generalthe dosimetrist and one of the physicists made the initialpass and the results from that pass were reviewed at a latertime by the second physicist The team met about once aweek to discuss and review ongoing progress Results fromthe dosimetristphysicists team were periodically evaluatedby one or two radiation oncologists based on the criterion ofclinical reasonableness that is given the planning contours astruth would the radiation oncologist judge the location andshape of the prostate in the tCT to be clinically reasonableThis criterion eliminated a potential source of interobserverbias and variability and effectively served the need for clinicalstandards Only a few tCTs per patient were reviewed becauseof the large number of cases and the fact that the positionand shape of the prostate in a given tCT are expected to bestrongly correlated with other tCTs for the same patient
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
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Active and Passive Electronic Components
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RotatingMachinery
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Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
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Shock and Vibration
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Civil EngineeringAdvances in
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Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
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Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
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Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
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Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
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Navigation and Observation
International Journal of
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DistributedSensor Networks
International Journal of
2 International Journal of Biomedical Imaging
Planned isocenter
(a)
Rigidly mapped isocenter
Nonrigidlymappedisocenter
(b)
Figure 1 (a) Axial slice from the pCT showing planning prostate (white) and isocenter (black) (b) Corresponding slice from the tCTshowing the prostate (black) segmented by automatic nonrigid model deformation The rigidly mapped isocenter comes from translatingthe planning prostate (dim white) to the tCT The nonrigidly mapped isocenter comes from applying the deformation matrix resulting fromautosegmentation to the planned isocenter
Table 1 Isocenter Mapping Methods
Clinical mapping Automatic mapping
1CT simulate Align patient with laser beams intersecting atsimulated isocenter Tattoo skin at centers of lateral and anteriorlaser beams
Import pCT structure sets and isocenter to MxAnatomy Fitmodels to planning contours
2 Plan Place crosshairs at planned isocenter in axial slice Markskin contour at lateral and anterior intersections with crosshairs Acquire tCT using standard procedures
3Prepare patient for treatment imaging Tape BBs to anterior andlateral skin tattoos Acquire tCT with laser beams centered onBBs
Import tCT Rigidly register pCT with pCT using automaticmultiscale procedure
4 Import tCT to PLanUNC Autoregister imaged BBs in tCT withskin marks in pCT from Step 2 Autosegment prostate in tCT
5Inspect registration by comparing prostate contours in pCTwith intensity patterns in the tCT Manually edit registration toget best match between contours and tCT intensities
Determine correspondences between pCT and tCT prostatemodels
6 Convert manual 119909 119910 119911 edits from Step 5 to table shifts relativeto laser beams Apply shifts gt3mm and treat
Map isocenter label from pCT to tCT via correspondence fromStep 5 (2)
scanner and the linac and a dual-purpose imagingtreatmentcouch that moves along the rails Patients under the IGRTprotocol were imaged before treatment and the couch wasrolled from the CT scanner into the image-guided treat-ment position The fixed geometry between the scanner andlinac allows cross calibration of the patient laser alignmentsystems and the rails facilitate moving the couch from thescanner into treatment position with minimal time delay ormechanical disturbance of patient geometry
All patients underwent simulation using a PhilipsAcQSim CT system [6] (Philips Healthcare Andover MA)The planning isocenter was localized during simulation andthe anterior and lateral laser crosshairs were tattooed accord-ing to standard practice Treatment planning and calculationof hypothetically delivered dose were accomplished withPlanUNC [7 8] (PLanUNC is a set of modular software toolsfor external beam treatment planning and dose calculation
development at UNC) During planning the dosimetristplaced the computer crosshairs at the planned isocenter andthen marked reference points in the pCT at the intersectionsof the computer crosshairs with the skin (Figure 2) Thesereference points defined the geometrically correct positionsof the anterior and lateral laser crosshairs based on patientgeometry at planning time Before acquisition of each tCTthe patient was positioned by aligning the tattoos on thepatientrsquos skin with the CT laser crosshairs After alignmentsteel BBs were taped to the skin at the center of eachlaserrsquos crosshairs (AP RampL lat) Assuming accurate lasercalibration this placement allows the treatment isocenter forthe initial patient position to be inferred from the imagedBBs Immediately after imaging the tCT was imported to theplanning system and the physicist defined the BB centers viapoint and click on a computer display screen The planningsystem then automatically registered the tCT and pCT by
International Journal of Biomedical Imaging 3
Planned isocenter
Ideal (marked)locations of BBs
(a)
Mapped isocenter
Imaged BBs
(b)
Figure 2 (a) Axial slice from the pCT showing planned isocenter inside the prostate (white contour) and the marked locations of BBs (b)Corresponding slice from the tCT showing the autosegmented prostate (black) nonrigidly mapped isocenter and imaged BBs
matching the BBs in the tCT with the ideal locations markedin the pCT The algorithm minimized sum(distance betweencorresponding points)2 The final step was interactive rigidregistration of the prostate ROIs using the planning contoursfor reference Table tilt around the lateral axis and rotationaround the craniocaudal axis were not allowed in the finaltwo steps because rotational errors were not handled duringpatient setup Since the prostate was not contoured in thetCT the final step relied on human judgment to match thepCT intensities and contours with the tCT intensity patternsin the prostate ROI Table displacements were computed bycomparing the coordinates of the mapped isocenter after BBregistration with the coordinates after interactive prostate-based registrationThe displacements were used to repositionthe treatment table Assuming accurate registration andrepositioning and no changes in patient anatomy betweentCT imaging and treatment times this procedure registeredthe mapped planned isocenter with the treatment isocenterIn typical practice of IGRT displacements are implementedonly when they exceed a predefined threshold In theUNC protocol the threshold was 3mm along a given axisHowever for comparison purposes this study assumed thatthe displacements were applied without error regardless ofmagnitude
22 Automatic MappingMethod Automapping (Table 1) wasperformed using a beta version of ARTSuite (MorphormicsInc Chapel Hill NC) installed at UNC (Effective July 162012 Morphormics Inc became a wholly owned subsidiaryof Accuray Inc Sunnyvale CA) ARTSuite is a DICOM-RTcompliant software system developed to support IGRT ARTand online reoptimization with tools for autosegmentationof pCTs and tCTs nonrigid mapping between treatment andplanning spaces and dose accumulation and analysis
Automapping (Figure 3) involved three major steps (1)multiscale rigid registration of the previously segmented pCTto the tCT (2)model-based autosegmentation of the prostatein the tCT [9 10] and (3) nonrigid mapping of the planningisocenter to the tCT using a transformation that includedthe rigid registration matrix and a nonstatistical nonrigiddiffeomorphism determined from correspondences betweenthe pCT and tCT prostate models
23 Patient Data Ten patients with a total of 243 tCTswere investigated All pCTs were acquired with contrast inthe bladder and one patient had contrast in the bladder andrectumThe pixel dimensions in the axial plane were 1mm times1mm and the slice thickness was 3mm for pCTs and tCTs
All patients were treatedwith step-and-shoot IMRTusingan anterior and six oblique fields to sim75Gy prescribed to apoint or isodose curve Treatment typically included a booststarting sim50Gy to reach the final dose Margins of 5mmand 3mm were applied to the planning target volume for theinitial and boost plans respectively
231 Model Fitting to Prostate Contours This study assumedthat the manually drawn prostate contours in the pCT weretrue at treatment time To facilitate model-based segmen-tation of the tCTs as described below a prostate modelwas fit to each set of planning contours using an approachbased on prostate shape statistics described by Merck et al[11] This process yielded a custom prostate atlas for eachpatient that was used during registration and segmentationof tCTs Contours were represented as many short linesegments joined together This representation caused smalldifferences between a contour and a model at sharp verticeswhere two line segments joined These differences wereless than 02mm per contour on average and were causedby smoothness constraints that forced the model to havecontinuous curvature
232Multiscale Rigid Registration Theoverall rigid registra-tion approach has similarities with that of Court and Dong[12] and Smitsmans et al [13] discussed later in Section 3 Tominimize compute time registration progresses from coarseto fine scale in three steps The output of each step serves as aprior for the following step Step (1) aligns the skin boundingboxes and registers the images by sliding the image data inthe bounding box in the pCT along the box for the tCT Theregistration algorithm computes the voxel count per slice in apredefined intensity window and aligns the images by findingthe best match between graphs of voxel count versus sliceposition for each image pair A bone window performs bestbut can fail when a ldquobrightrdquo contrast medium is used for thepCT In such cases Step (1) is ignored and the algorithm starts
4 International Journal of Biomedical Imaging
(a) (b)
(c) (d)
(e) (f)
Figure 3 Multiscale registration of a pCT with a CBCT The planning prostate segmentation is white ((a) (b)) Blended axial and sagittalslices of unregistered images ((c) (d)) Axial and sagittal slices of images registered via Step (1) ((e) (f)) Axial and sagittal slices of imagesregistered via mutual information in the prostate ROI (Step (3)) In this example there is little difference between the second and third steps
over at Step (2) which optimizes global mutual information(MI) using a gradient descent approach [14] To avoid con-vergence to a distant optimum the algorithm is run multipletimes with different starting points The result with the bestscore over all runs is selected as the output Step (3) is similar
to Step (2) but with MI computed over an ROI defined by theatlas prostate model As in the clinical procedure rotationsduring automatic registration were not allowed explicitlyHowever the segmentation step treated rotation as a nonrigiddeformation in images with adequate intensity information
International Journal of Biomedical Imaging 5
Rigidly registered prostate model
Deformedprostatemodel
Gas bubble
Bone overlap
Figure 4 Midsagittal slice from a tCT illustrating how prostaterotation is treated as a deformation The white outline is the atlasprostate after automatic registration to the tCTThe black dashes arethe deformed atlas in the tCT
In Figure 4 for example the rigidly registered prostatemodeloverlaps pubic bone anteriorly causing the model to deformin a manner that avoids overlap with both the bone and thegas bubble in the rectum
233 Model-Based Autosegmentation The model used torepresent the prostate consists of a chain of so-called medialatoms (Figure 5) A full collection of atoms for an organis called a medial-representation (m-rep) [9] The chainconfiguration is well suited for objects that are more or lesstube-like including objects with closed ends Each prostateatom has a hub and 16 spokes radiating to the organsurface Additional hubs and spokes can be interpolated asneeded The skeletal framework serves as an organ-relativecoordinate system with a formalism for converting backand forth between model and image coordinates [9 15]After deformation of the starting model in a target imagecorresponding positions are defined by pairing points in thestarting and deformed models that have the same model-relative coordinates (Figure 5) The nonrigid transformationmatrix can be specified in image coordinates in terms of astandard displacement vector field [16] where each vectororiginates on a voxel in the reference image and terminates onits postdeformation position in the target image In contrastto voxel-scale deformations the model approach is statisticalat the scale of an organ but nonstatistical at voxel scaleeliminating small-scale artifacts [16]
Segmentation of the prostate in the tCT is necessaryto determine corresponding points in the pCT and tCTThe algorithm transfers the atlas model to the tCT usingthe rigid registration matrix and autosegmentation proceedsin a statistical framework based on Bayesrsquo theorem [9] Aconjugate gradient algorithm seeks to find the optimal model119872opt such that
119872opt = argmax119872isin119904
[log119901 (119872) + log119901 (119868 | 119872)] (1)
where 119872 is the currently deformed model in the trainedshape space 119904 [11] 119868 is the target image intensity patternrelative to 119872 119901(119872) is the probability of 119872 (geometrictypicality) and 119901(119868 |119872) is the probability of 119868 given119872 (imagematch [17])
234 Mapping the Isocenter The rationale for using a modelto map the isocenter stems from several considerations (1)during planning the isocenter is positioned relative to theprostate (2) a point in an image can be more accuratelyfoundby relying on regional image features that are correlatedspatially with the point rather than using local informationnear the point itself [18] and (3) the trainable models usedin this study provide a means for determining both the rigidand nonrigid components of the mapping transformationThe mapping step is straightforward and involves labelingthe point in the tCT that has the same prostate-relativecoordinates as the planned isocenter using (2)
VAL1015840Mapped (1198721015840(1198941015840 1198951015840 1198961015840)) = VAL (119872 (119894 119895 119896)) (2)
where 119872 1198721015840 = prostate models in pCT and tCT respec-tively 119894 119895 119896 and 1198941015840 1198951015840 1198961015840 are corresponding positions in119872- and 1198721015840-relative coordinates VAL = value of scalar forexample label dose or intensity in the pCT at 119872-relativeposition 119894 119895 119896 and VAL1015840Mapped = value of scalar mapped to1198721015840-relative position 1198941015840 1198951015840 1198961015840
24 Reference tCT Isocenters The clinical and automappingprotocols yielded two independent sets of tCT isocentersTo compare these sets a reference isocenter was determinedfor each tCT by repeating the automapping procedure withhuman supervision The main task was to reposition andoredit the autosegmented prostate as necessary to achieve thebest match with the tCT image data while generally preserv-ing the global shape and volume defined by the planningcontours Every rigid registration and prostate segmentationwere evaluated and edited based on human judgment afterwhich the tCT isocenter from (2) was accepted withoutmodification This procedure was performed without thepressure of clinical time constraints over sim8 months by twophysicists and a dosimetrist working as a team In generalthe dosimetrist and one of the physicists made the initialpass and the results from that pass were reviewed at a latertime by the second physicist The team met about once aweek to discuss and review ongoing progress Results fromthe dosimetristphysicists team were periodically evaluatedby one or two radiation oncologists based on the criterion ofclinical reasonableness that is given the planning contours astruth would the radiation oncologist judge the location andshape of the prostate in the tCT to be clinically reasonableThis criterion eliminated a potential source of interobserverbias and variability and effectively served the need for clinicalstandards Only a few tCTs per patient were reviewed becauseof the large number of cases and the fact that the positionand shape of the prostate in a given tCT are expected to bestrongly correlated with other tCTs for the same patient
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
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Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
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International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Biomedical Imaging 3
Planned isocenter
Ideal (marked)locations of BBs
(a)
Mapped isocenter
Imaged BBs
(b)
Figure 2 (a) Axial slice from the pCT showing planned isocenter inside the prostate (white contour) and the marked locations of BBs (b)Corresponding slice from the tCT showing the autosegmented prostate (black) nonrigidly mapped isocenter and imaged BBs
matching the BBs in the tCT with the ideal locations markedin the pCT The algorithm minimized sum(distance betweencorresponding points)2 The final step was interactive rigidregistration of the prostate ROIs using the planning contoursfor reference Table tilt around the lateral axis and rotationaround the craniocaudal axis were not allowed in the finaltwo steps because rotational errors were not handled duringpatient setup Since the prostate was not contoured in thetCT the final step relied on human judgment to match thepCT intensities and contours with the tCT intensity patternsin the prostate ROI Table displacements were computed bycomparing the coordinates of the mapped isocenter after BBregistration with the coordinates after interactive prostate-based registrationThe displacements were used to repositionthe treatment table Assuming accurate registration andrepositioning and no changes in patient anatomy betweentCT imaging and treatment times this procedure registeredthe mapped planned isocenter with the treatment isocenterIn typical practice of IGRT displacements are implementedonly when they exceed a predefined threshold In theUNC protocol the threshold was 3mm along a given axisHowever for comparison purposes this study assumed thatthe displacements were applied without error regardless ofmagnitude
22 Automatic MappingMethod Automapping (Table 1) wasperformed using a beta version of ARTSuite (MorphormicsInc Chapel Hill NC) installed at UNC (Effective July 162012 Morphormics Inc became a wholly owned subsidiaryof Accuray Inc Sunnyvale CA) ARTSuite is a DICOM-RTcompliant software system developed to support IGRT ARTand online reoptimization with tools for autosegmentationof pCTs and tCTs nonrigid mapping between treatment andplanning spaces and dose accumulation and analysis
Automapping (Figure 3) involved three major steps (1)multiscale rigid registration of the previously segmented pCTto the tCT (2)model-based autosegmentation of the prostatein the tCT [9 10] and (3) nonrigid mapping of the planningisocenter to the tCT using a transformation that includedthe rigid registration matrix and a nonstatistical nonrigiddiffeomorphism determined from correspondences betweenthe pCT and tCT prostate models
23 Patient Data Ten patients with a total of 243 tCTswere investigated All pCTs were acquired with contrast inthe bladder and one patient had contrast in the bladder andrectumThe pixel dimensions in the axial plane were 1mm times1mm and the slice thickness was 3mm for pCTs and tCTs
All patients were treatedwith step-and-shoot IMRTusingan anterior and six oblique fields to sim75Gy prescribed to apoint or isodose curve Treatment typically included a booststarting sim50Gy to reach the final dose Margins of 5mmand 3mm were applied to the planning target volume for theinitial and boost plans respectively
231 Model Fitting to Prostate Contours This study assumedthat the manually drawn prostate contours in the pCT weretrue at treatment time To facilitate model-based segmen-tation of the tCTs as described below a prostate modelwas fit to each set of planning contours using an approachbased on prostate shape statistics described by Merck et al[11] This process yielded a custom prostate atlas for eachpatient that was used during registration and segmentationof tCTs Contours were represented as many short linesegments joined together This representation caused smalldifferences between a contour and a model at sharp verticeswhere two line segments joined These differences wereless than 02mm per contour on average and were causedby smoothness constraints that forced the model to havecontinuous curvature
232Multiscale Rigid Registration Theoverall rigid registra-tion approach has similarities with that of Court and Dong[12] and Smitsmans et al [13] discussed later in Section 3 Tominimize compute time registration progresses from coarseto fine scale in three steps The output of each step serves as aprior for the following step Step (1) aligns the skin boundingboxes and registers the images by sliding the image data inthe bounding box in the pCT along the box for the tCT Theregistration algorithm computes the voxel count per slice in apredefined intensity window and aligns the images by findingthe best match between graphs of voxel count versus sliceposition for each image pair A bone window performs bestbut can fail when a ldquobrightrdquo contrast medium is used for thepCT In such cases Step (1) is ignored and the algorithm starts
4 International Journal of Biomedical Imaging
(a) (b)
(c) (d)
(e) (f)
Figure 3 Multiscale registration of a pCT with a CBCT The planning prostate segmentation is white ((a) (b)) Blended axial and sagittalslices of unregistered images ((c) (d)) Axial and sagittal slices of images registered via Step (1) ((e) (f)) Axial and sagittal slices of imagesregistered via mutual information in the prostate ROI (Step (3)) In this example there is little difference between the second and third steps
over at Step (2) which optimizes global mutual information(MI) using a gradient descent approach [14] To avoid con-vergence to a distant optimum the algorithm is run multipletimes with different starting points The result with the bestscore over all runs is selected as the output Step (3) is similar
to Step (2) but with MI computed over an ROI defined by theatlas prostate model As in the clinical procedure rotationsduring automatic registration were not allowed explicitlyHowever the segmentation step treated rotation as a nonrigiddeformation in images with adequate intensity information
International Journal of Biomedical Imaging 5
Rigidly registered prostate model
Deformedprostatemodel
Gas bubble
Bone overlap
Figure 4 Midsagittal slice from a tCT illustrating how prostaterotation is treated as a deformation The white outline is the atlasprostate after automatic registration to the tCTThe black dashes arethe deformed atlas in the tCT
In Figure 4 for example the rigidly registered prostatemodeloverlaps pubic bone anteriorly causing the model to deformin a manner that avoids overlap with both the bone and thegas bubble in the rectum
233 Model-Based Autosegmentation The model used torepresent the prostate consists of a chain of so-called medialatoms (Figure 5) A full collection of atoms for an organis called a medial-representation (m-rep) [9] The chainconfiguration is well suited for objects that are more or lesstube-like including objects with closed ends Each prostateatom has a hub and 16 spokes radiating to the organsurface Additional hubs and spokes can be interpolated asneeded The skeletal framework serves as an organ-relativecoordinate system with a formalism for converting backand forth between model and image coordinates [9 15]After deformation of the starting model in a target imagecorresponding positions are defined by pairing points in thestarting and deformed models that have the same model-relative coordinates (Figure 5) The nonrigid transformationmatrix can be specified in image coordinates in terms of astandard displacement vector field [16] where each vectororiginates on a voxel in the reference image and terminates onits postdeformation position in the target image In contrastto voxel-scale deformations the model approach is statisticalat the scale of an organ but nonstatistical at voxel scaleeliminating small-scale artifacts [16]
Segmentation of the prostate in the tCT is necessaryto determine corresponding points in the pCT and tCTThe algorithm transfers the atlas model to the tCT usingthe rigid registration matrix and autosegmentation proceedsin a statistical framework based on Bayesrsquo theorem [9] Aconjugate gradient algorithm seeks to find the optimal model119872opt such that
119872opt = argmax119872isin119904
[log119901 (119872) + log119901 (119868 | 119872)] (1)
where 119872 is the currently deformed model in the trainedshape space 119904 [11] 119868 is the target image intensity patternrelative to 119872 119901(119872) is the probability of 119872 (geometrictypicality) and 119901(119868 |119872) is the probability of 119868 given119872 (imagematch [17])
234 Mapping the Isocenter The rationale for using a modelto map the isocenter stems from several considerations (1)during planning the isocenter is positioned relative to theprostate (2) a point in an image can be more accuratelyfoundby relying on regional image features that are correlatedspatially with the point rather than using local informationnear the point itself [18] and (3) the trainable models usedin this study provide a means for determining both the rigidand nonrigid components of the mapping transformationThe mapping step is straightforward and involves labelingthe point in the tCT that has the same prostate-relativecoordinates as the planned isocenter using (2)
VAL1015840Mapped (1198721015840(1198941015840 1198951015840 1198961015840)) = VAL (119872 (119894 119895 119896)) (2)
where 119872 1198721015840 = prostate models in pCT and tCT respec-tively 119894 119895 119896 and 1198941015840 1198951015840 1198961015840 are corresponding positions in119872- and 1198721015840-relative coordinates VAL = value of scalar forexample label dose or intensity in the pCT at 119872-relativeposition 119894 119895 119896 and VAL1015840Mapped = value of scalar mapped to1198721015840-relative position 1198941015840 1198951015840 1198961015840
24 Reference tCT Isocenters The clinical and automappingprotocols yielded two independent sets of tCT isocentersTo compare these sets a reference isocenter was determinedfor each tCT by repeating the automapping procedure withhuman supervision The main task was to reposition andoredit the autosegmented prostate as necessary to achieve thebest match with the tCT image data while generally preserv-ing the global shape and volume defined by the planningcontours Every rigid registration and prostate segmentationwere evaluated and edited based on human judgment afterwhich the tCT isocenter from (2) was accepted withoutmodification This procedure was performed without thepressure of clinical time constraints over sim8 months by twophysicists and a dosimetrist working as a team In generalthe dosimetrist and one of the physicists made the initialpass and the results from that pass were reviewed at a latertime by the second physicist The team met about once aweek to discuss and review ongoing progress Results fromthe dosimetristphysicists team were periodically evaluatedby one or two radiation oncologists based on the criterion ofclinical reasonableness that is given the planning contours astruth would the radiation oncologist judge the location andshape of the prostate in the tCT to be clinically reasonableThis criterion eliminated a potential source of interobserverbias and variability and effectively served the need for clinicalstandards Only a few tCTs per patient were reviewed becauseof the large number of cases and the fact that the positionand shape of the prostate in a given tCT are expected to bestrongly correlated with other tCTs for the same patient
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
4 International Journal of Biomedical Imaging
(a) (b)
(c) (d)
(e) (f)
Figure 3 Multiscale registration of a pCT with a CBCT The planning prostate segmentation is white ((a) (b)) Blended axial and sagittalslices of unregistered images ((c) (d)) Axial and sagittal slices of images registered via Step (1) ((e) (f)) Axial and sagittal slices of imagesregistered via mutual information in the prostate ROI (Step (3)) In this example there is little difference between the second and third steps
over at Step (2) which optimizes global mutual information(MI) using a gradient descent approach [14] To avoid con-vergence to a distant optimum the algorithm is run multipletimes with different starting points The result with the bestscore over all runs is selected as the output Step (3) is similar
to Step (2) but with MI computed over an ROI defined by theatlas prostate model As in the clinical procedure rotationsduring automatic registration were not allowed explicitlyHowever the segmentation step treated rotation as a nonrigiddeformation in images with adequate intensity information
International Journal of Biomedical Imaging 5
Rigidly registered prostate model
Deformedprostatemodel
Gas bubble
Bone overlap
Figure 4 Midsagittal slice from a tCT illustrating how prostaterotation is treated as a deformation The white outline is the atlasprostate after automatic registration to the tCTThe black dashes arethe deformed atlas in the tCT
In Figure 4 for example the rigidly registered prostatemodeloverlaps pubic bone anteriorly causing the model to deformin a manner that avoids overlap with both the bone and thegas bubble in the rectum
233 Model-Based Autosegmentation The model used torepresent the prostate consists of a chain of so-called medialatoms (Figure 5) A full collection of atoms for an organis called a medial-representation (m-rep) [9] The chainconfiguration is well suited for objects that are more or lesstube-like including objects with closed ends Each prostateatom has a hub and 16 spokes radiating to the organsurface Additional hubs and spokes can be interpolated asneeded The skeletal framework serves as an organ-relativecoordinate system with a formalism for converting backand forth between model and image coordinates [9 15]After deformation of the starting model in a target imagecorresponding positions are defined by pairing points in thestarting and deformed models that have the same model-relative coordinates (Figure 5) The nonrigid transformationmatrix can be specified in image coordinates in terms of astandard displacement vector field [16] where each vectororiginates on a voxel in the reference image and terminates onits postdeformation position in the target image In contrastto voxel-scale deformations the model approach is statisticalat the scale of an organ but nonstatistical at voxel scaleeliminating small-scale artifacts [16]
Segmentation of the prostate in the tCT is necessaryto determine corresponding points in the pCT and tCTThe algorithm transfers the atlas model to the tCT usingthe rigid registration matrix and autosegmentation proceedsin a statistical framework based on Bayesrsquo theorem [9] Aconjugate gradient algorithm seeks to find the optimal model119872opt such that
119872opt = argmax119872isin119904
[log119901 (119872) + log119901 (119868 | 119872)] (1)
where 119872 is the currently deformed model in the trainedshape space 119904 [11] 119868 is the target image intensity patternrelative to 119872 119901(119872) is the probability of 119872 (geometrictypicality) and 119901(119868 |119872) is the probability of 119868 given119872 (imagematch [17])
234 Mapping the Isocenter The rationale for using a modelto map the isocenter stems from several considerations (1)during planning the isocenter is positioned relative to theprostate (2) a point in an image can be more accuratelyfoundby relying on regional image features that are correlatedspatially with the point rather than using local informationnear the point itself [18] and (3) the trainable models usedin this study provide a means for determining both the rigidand nonrigid components of the mapping transformationThe mapping step is straightforward and involves labelingthe point in the tCT that has the same prostate-relativecoordinates as the planned isocenter using (2)
VAL1015840Mapped (1198721015840(1198941015840 1198951015840 1198961015840)) = VAL (119872 (119894 119895 119896)) (2)
where 119872 1198721015840 = prostate models in pCT and tCT respec-tively 119894 119895 119896 and 1198941015840 1198951015840 1198961015840 are corresponding positions in119872- and 1198721015840-relative coordinates VAL = value of scalar forexample label dose or intensity in the pCT at 119872-relativeposition 119894 119895 119896 and VAL1015840Mapped = value of scalar mapped to1198721015840-relative position 1198941015840 1198951015840 1198961015840
24 Reference tCT Isocenters The clinical and automappingprotocols yielded two independent sets of tCT isocentersTo compare these sets a reference isocenter was determinedfor each tCT by repeating the automapping procedure withhuman supervision The main task was to reposition andoredit the autosegmented prostate as necessary to achieve thebest match with the tCT image data while generally preserv-ing the global shape and volume defined by the planningcontours Every rigid registration and prostate segmentationwere evaluated and edited based on human judgment afterwhich the tCT isocenter from (2) was accepted withoutmodification This procedure was performed without thepressure of clinical time constraints over sim8 months by twophysicists and a dosimetrist working as a team In generalthe dosimetrist and one of the physicists made the initialpass and the results from that pass were reviewed at a latertime by the second physicist The team met about once aweek to discuss and review ongoing progress Results fromthe dosimetristphysicists team were periodically evaluatedby one or two radiation oncologists based on the criterion ofclinical reasonableness that is given the planning contours astruth would the radiation oncologist judge the location andshape of the prostate in the tCT to be clinically reasonableThis criterion eliminated a potential source of interobserverbias and variability and effectively served the need for clinicalstandards Only a few tCTs per patient were reviewed becauseof the large number of cases and the fact that the positionand shape of the prostate in a given tCT are expected to bestrongly correlated with other tCTs for the same patient
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
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RoboticsJournal of
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Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Biomedical Imaging 5
Rigidly registered prostate model
Deformedprostatemodel
Gas bubble
Bone overlap
Figure 4 Midsagittal slice from a tCT illustrating how prostaterotation is treated as a deformation The white outline is the atlasprostate after automatic registration to the tCTThe black dashes arethe deformed atlas in the tCT
In Figure 4 for example the rigidly registered prostatemodeloverlaps pubic bone anteriorly causing the model to deformin a manner that avoids overlap with both the bone and thegas bubble in the rectum
233 Model-Based Autosegmentation The model used torepresent the prostate consists of a chain of so-called medialatoms (Figure 5) A full collection of atoms for an organis called a medial-representation (m-rep) [9] The chainconfiguration is well suited for objects that are more or lesstube-like including objects with closed ends Each prostateatom has a hub and 16 spokes radiating to the organsurface Additional hubs and spokes can be interpolated asneeded The skeletal framework serves as an organ-relativecoordinate system with a formalism for converting backand forth between model and image coordinates [9 15]After deformation of the starting model in a target imagecorresponding positions are defined by pairing points in thestarting and deformed models that have the same model-relative coordinates (Figure 5) The nonrigid transformationmatrix can be specified in image coordinates in terms of astandard displacement vector field [16] where each vectororiginates on a voxel in the reference image and terminates onits postdeformation position in the target image In contrastto voxel-scale deformations the model approach is statisticalat the scale of an organ but nonstatistical at voxel scaleeliminating small-scale artifacts [16]
Segmentation of the prostate in the tCT is necessaryto determine corresponding points in the pCT and tCTThe algorithm transfers the atlas model to the tCT usingthe rigid registration matrix and autosegmentation proceedsin a statistical framework based on Bayesrsquo theorem [9] Aconjugate gradient algorithm seeks to find the optimal model119872opt such that
119872opt = argmax119872isin119904
[log119901 (119872) + log119901 (119868 | 119872)] (1)
where 119872 is the currently deformed model in the trainedshape space 119904 [11] 119868 is the target image intensity patternrelative to 119872 119901(119872) is the probability of 119872 (geometrictypicality) and 119901(119868 |119872) is the probability of 119868 given119872 (imagematch [17])
234 Mapping the Isocenter The rationale for using a modelto map the isocenter stems from several considerations (1)during planning the isocenter is positioned relative to theprostate (2) a point in an image can be more accuratelyfoundby relying on regional image features that are correlatedspatially with the point rather than using local informationnear the point itself [18] and (3) the trainable models usedin this study provide a means for determining both the rigidand nonrigid components of the mapping transformationThe mapping step is straightforward and involves labelingthe point in the tCT that has the same prostate-relativecoordinates as the planned isocenter using (2)
VAL1015840Mapped (1198721015840(1198941015840 1198951015840 1198961015840)) = VAL (119872 (119894 119895 119896)) (2)
where 119872 1198721015840 = prostate models in pCT and tCT respec-tively 119894 119895 119896 and 1198941015840 1198951015840 1198961015840 are corresponding positions in119872- and 1198721015840-relative coordinates VAL = value of scalar forexample label dose or intensity in the pCT at 119872-relativeposition 119894 119895 119896 and VAL1015840Mapped = value of scalar mapped to1198721015840-relative position 1198941015840 1198951015840 1198961015840
24 Reference tCT Isocenters The clinical and automappingprotocols yielded two independent sets of tCT isocentersTo compare these sets a reference isocenter was determinedfor each tCT by repeating the automapping procedure withhuman supervision The main task was to reposition andoredit the autosegmented prostate as necessary to achieve thebest match with the tCT image data while generally preserv-ing the global shape and volume defined by the planningcontours Every rigid registration and prostate segmentationwere evaluated and edited based on human judgment afterwhich the tCT isocenter from (2) was accepted withoutmodification This procedure was performed without thepressure of clinical time constraints over sim8 months by twophysicists and a dosimetrist working as a team In generalthe dosimetrist and one of the physicists made the initialpass and the results from that pass were reviewed at a latertime by the second physicist The team met about once aweek to discuss and review ongoing progress Results fromthe dosimetristphysicists team were periodically evaluatedby one or two radiation oncologists based on the criterion ofclinical reasonableness that is given the planning contours astruth would the radiation oncologist judge the location andshape of the prostate in the tCT to be clinically reasonableThis criterion eliminated a potential source of interobserverbias and variability and effectively served the need for clinicalstandards Only a few tCTs per patient were reviewed becauseof the large number of cases and the fact that the positionand shape of the prostate in a given tCT are expected to bestrongly correlated with other tCTs for the same patient
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
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Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
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Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
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Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
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Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
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Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
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Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
6 International Journal of Biomedical Imaging
Base
Apex
Ant
ase
Apex
Ant
(a)
Hub
Spokes
b
Spokes
(b)
origin
i j k
(c)
i998400 j998400 k998400
origin998400
(d)
Figure 5 (a) Lateral oblique view of the surface of a prostatemodel (b) Internal tubular skeleton showing a chain of 13 atoms each comprisinga hub and 16 spokes that touch the prostate surface (c) and (d) Illustration of corresponding points in reference and deformed models (c)Reference model with point at 119894 119895 119896 (d) Deformed model with corresponding point at 1198941015840 1198951015840 1198961015840 The points are on the same spoke and theyhave the same fractional distance from the origin (atom hub)
(a) (b)
minus25 cGy
minus50 cGy
minus100 cGy
(c) (d)
Figure 6 Organ contours and isodose curves on midsagittal slices for a typical case Organs shown are the prostate (red) seminal vesicles(green) bladder (blue) rectum (yellow) and anterior rectal wall (purple) (a) Planned isodoses on pCT (b) Cumulative isodoses on pCT (c)Error dose on pCT (d) Delivered isodoses computed from one tCT
25 Calculation of Hypothetical Delivered Dose DistributionsTreatment dose distributions for each tCT and each mappedisocenter were computed using PlanUNC assuming all beamswere delivered as planned for each of the three isocenters(Figure 6) This was accomplished by importing each tCTto PlanUNC registering the ensemble of planned beams toeach of the treatment isocenters in turn and calculating
the delivered dose assuming all beams were delivered asplanned After dose calculation the DICOM-RT files for theplanned and treatment dose distributions were imported toARTSuite and dose distributions were mapped from tCTsto the pCT using (2) in the reverse direction Except for arind sim2ndash5mm thick around the prostate dose to interstitialtissues was not mapped since (2) applies only to modeled
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Biomedical Imaging 7
0
10
20
30
40
Dose (cGy)
Volu
me (
)
minus85 minus75 minus65 minus55 minus45 minus35 minus25 minus15 minus5
Figure 7 Prostate DVH for the error dose distribution shown inFigure 6(c) The bin size is 10 cGy
tissues Dose to the rind was mapped by extrapolating theskeletal framework a small distance beyond the prostatesurface The mapped treatment doses were summed overall tCTs and all isocenters and resampled to the grid ofthe planning dose to simplify comparison of planned andtreatment dose distributions Figure 6(a) shows the plannedisodose curves for the 10 25 50 85 90 and 95 levels onthe pCT for the initial (nonboost) portionThe proximal twoslices (6mm length) of the seminal vesicles were included inthe PTV Figure 6(b) shows the same isodose levels from thecumulative dose for the clinical protocol over 15 fractionsError dose distributions (Figure 6(c)) were computed bysubtracting the scaled planned dose distribution from thesummed treatment dose distribution The scaling factor wasdetermined by the number of fractions contributing to thesummed treatment dose Isodose curves are shown for minus100minus50 and minus25 cGy Figure 6(d) shows the same isodose levelsas in Figure 6(a) computed from one of the 15 tCTs Thefrequency distribution in Figure 7 illustrates the expectedunderdosing of the prostate due to differences betweenprostate shape and location at planning and treatment times
For dose accumulation purposes the spatial accuracyrequired for nonrigid registration of a point in the tCTwith its corresponding point in the pCT depends on thetolerable dose error and the steepness of dose gradients nearthe points Assuming that the spacing between calculationpoints in the dose grid is matched to the dose gradients[19 20] correspondence errors should be small comparedto the grid spacing The clinical planning grid spacing was5mm in this study Figure 8 shows color-coded maps ofdifferences between the positions of two points one point foreach method resulting from a single point in the tCT Thedifferences were sim1mm along the 119909 and 119910 axes and sim2mmalong the 119911 axis for the prostate ROI The larger differencealong the 119911 axis is attributed to the 3mmslice thicknessThesefindings support the use of m-reps for dose accumulation forthis study
3 Results
31 Distance Metrics Frequency histograms (Figure 9)were computed from the signed differences (Δ119909 Δ119910 Δ119911)
(Figure 10) between the reference isocenters and the clinicaland automatic isocenters for all 243 tCTs The bin widthfor Δ119909 and Δ119910 was 05mm To maintain comparablecounts per bin the width for Δ119911 was chosen to be 10mmSummary statistics for all ten patients are given in Table 2Figure 9 shows that the distributions for clinical andautomatic isocenters are centered near the reference valuesin approximately Gaussian fashion supporting the utility ofthe reference values
Comparison of the frequency histograms for clinicaland automatic protocols shows that automatic mapping isrobust as accurate as the clinical protocol along all threeaxes and more precise than the clinical protocol whereaccuracy is the average of the unsigned Δ119904 compared tothe reference values and precision is the spread (standarddeviation) for each axis Even though the averages for theautomatic method are smaller (closer to the references) thanthe clinical protocol greater accuracy is not claimed becausethe references are not goldenOn the other hand the standarddeviation is characteristic of the registration method andindependent of the reference values The ANOVA 119865-test islt10minus12 for all three axes demonstrating that human and
automatic variances are significantly different As seen fromTable 2 these observations apply for each individual patientMoreover the clinical protocol yielded 8 outliers definedhere as differences gt3120590clinical (120590clinical = standard deviation ofclinical protocol) with the largest being almost 5120590clinical Incomparison the largest difference for the automatic approachis slightly less than 3120590clinical along the 119909 axis for patient 10 andfor this case 120590clinical is small (asymp1mm)
Table 2 also gives results for Court and Dong [12] andSmitsmans et al [13] Both studies evaluated automaticlocalization of the prostate in tCTs via multiscale rigidregistration with pCTs The values given in Table 2 for thesestudies are differences in prostate position as opposed toisocenter position between automaticmethods andmanuallyprepared references Court and Dong reported results fortwo patients patient A had 22 tCTs and was considered lesschallenging than patient B who had 21 tCTs Smitsmans etal looked at a collection of 19 patients with 8ndash13 tCTs eachThe results in Table 2 are for 91 of the tCTs The remaining9were considered outliers and quantitative results were notreported The automatic rigid registration method presentedin this paper appears qualitatively to be comparable inperformance to both Court and Dong and Smitsmans et alNo direct quantitative comparisons are possible however dueto differences in study designs
32 Prostate DVHs
321 Initial Portion of Treatment Regimen Prostate DVHsfor doses accumulated using the clinical automatic andreference isocenters for two typical patients are comparedagainst the scaled planned DVHs in Figure 11 These casesillustrate (i) small differences among the three isocenters (ii)degradation of the shoulder region and (iii) a decrease indelivered versus planned dose of sim100ndash200 cGy scaled to thefull nonboost portionThese general findings were consistent
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
8 International Journal of Biomedical Imaging
Table2Summarysta
tistic
sovera
llpatie
nts
Patie
ntΔ119883(m
m)
Δ119884(m
m)
Δ119885(m
m)
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
|Av
g|dagger
MaxM
inStdDev
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
Clinic
Auto
113
04
28minus30
17minus
02
1505
23
1467minus60
02minus58
30
1732
12yen 129minus22
35minus14
41
142
1104
31minus16
12minus
07
1305
1409
48minus42
20minus24
1811
1906
64minus66
25minus22
27
09
311
05
17minus
34
17minus
09
1406
1909
18minus
61
20minus40
22
1317
1027minus49
35minus21
21
134
1006
28minus36
28minus13
1408
1710
yen 117
minus68
05minus49
29
1327
08
yen 184minus65
11minus
31
42
115
07
06
24minus15
12minus
1209
07
1409
29minus44
08minus47
1712
23
15yen 112
minus22
45minus17
30
176
08
04
21minus16
06minus22
1005
1510
37minus43
25minus33
1913
30
11104minus
48
33minus23
36
147
1207
27minus35
02minus23
1508
1809
32minus52
21minus23
22
1120
08
yen 118
minus14
28minus47
27
128
09
03
32minus18
09minus12
1203
1407
33
yen minus62
08minus24
1808
1808
yen 140minus25
32minus19
28
119
09
06
3305
18minus
04
1006
1408
30minus48
19minus
1319
09
29
08
44minus91
41minus13
36
1110
07
06
29minus21
09minus31
1008
1008
46minus13
35minus20
1312
20
1353minus60
39minus16
26
15All
1106
33minus36
28minus31
1408
1811
117minus68
35minus58
23
1525
11yen 184minus91
45minus47
35
14Re
ference[12]P
atA
NAlowast
00
10+
05
NAlowast
02
11+
05
NAlowast
03
24+
10Re
ference[12]P
atB
NAlowast
03
14+
06
NAlowastminus02
19+
14NAlowastminus01
35+
19Re
ference[13]
NAlowast
01
07
NAlowast
01
12NAlowast
00
13yen B
oldvalues
areo
utliersdaggerAv
erageo
funsigneddifferenceslowastNot
applicable
+ Maxim
umAv
erageo
fsigneddifferences
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Biomedical Imaging 9
20
100 200
40
60300
02
0
minus02
RL
(a)
20
40
60100 200 300
02
0
minus02
04PA
(b)
20
100 200
02
0
minus02
04
06IS
40
60300
(c)
Figure 8 Color-coded difference maps for points in the tCT nonrigidly registered to the pCT using FEM and models In the prostate ROIthe agreement between the two methods is sim1mm along the 119909 and 119910 axes and sim2mm along the 119911 axis The larger difference along the 119911 axisis attributed to the 3mm slice thickness
0
10
20
30
40
50
60
70
80
90
minus4 minus3 minus2 minus1 0 1 2 3 4
Cou
nt
Black = clinicalGray = automatic
Δx (mm)
(a)
minus6 minus5 minus4 minus3 minus2 minus10
5
10
15
20
25
30
35
40
0 1 2 3 4 5 6
Cou
nt
Black = clinicalGray = automatic
Δy (mm)
(b)
102030405060708090
minus6 minus4 minus20
0 2 4
100
minus10 minus8 6 8 10
Cou
nt
Black = clinicalGray = automatic
Δz (mm)
(c)
Figure 9 Frequency histograms for Δ119909 Δ119910 and Δ119911 The averages of the unsigned clinical values for Δ119909 Δ119910 and Δ119911 respectively are106mm 179mm and 254mmThe averages of the automatic values are 058mm 114mm and 105mm Two clinical values are outside theΔ119910 axis range and seven values are outside the Δ119911 range All of the automatic results are within the ranges of all axes
across all ten patients but the severity of shoulder degra-dation was patient specific Automatic mapping performedbetter in the shoulder region (Figure 11(a)) than the clinicalprotocol in about half the cases and as well in the other half(Figure 11(b)) The absence of more significant differences is
attributed to margins (5mm) that were relatively insensitiveto isocenter mapping variations on the order of a few mm afinding expected for properly designed margins
Figure 7 shows the differential DVH for the error dose forthe patient in Figure 11(a) Error isodose curves in Figure 6(c)
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
10 International Journal of Biomedical Imaging
minusx
minusz
+x
+z
(a)
minusz
minusy
+z
+y
(b)
Figure 10 Coordinate system for calculating Δ119909 Δ119910 and Δ119911
0
20
40
60
80
100
2400 2600 2800 3000 3200
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
(a)
PlannedClinical
AutoReference
Dose (cGy)
0
20
40
60
80
100
1700 1900 2100 2300 2500 2700
Volu
me (
)
(b)
Figure 11 Prostate accumulated-dose DVHs for two patients The planned doses have been scaled to the number of fractions accumulatedfor each patient
show that the underdosed region occurs at the apex Thesuperior shift of the delivered dose distribution displayedon the tCT in Figure 6(d) was also present on other tCTsexplaining the origin of the under dose Underdosing atthe base was not observed for this patient because theplanning target volume was enlarged superiorly to includethe proximal SVs providing extra protection at the baseHowever underdosing was observed at both the base andapex for all patients whose SVswere not included in the targetvolume
322 Boost Portion of Treatment Regimen TCTs for boostfractions were available for only two patients DVHs inFigure 12 were computed from tCTs acquired for four oftwelve boost fractions The DVHs for both patients show thesame general trends observed for the initial treatment por-tion (Figure 11) However the clear separation between thedescending portions of the clinical and automatic isocenters
in Figure 12 suggests that automatic mapping may reduce theoverall prostate under dose compared to the clinical protocolIf true this finding would not be surprising since the boostmargin (3mm) would be expected to be more sensitive toimage registration errors However further study is neededto test this finding
4 Discussion and Conclusions
This work presents a formalism for mapping the plannedisocenter to a tCT based on correspondence properties of adeformable prostate organ model that is used for registrationof the pCT and tCT and for segmentation of the prostate inthe tCTThe fully automaticmapping algorithm is as accurateas the clinical protocol but more precise The algorithm hadno failures or outliers for the tCTs studied Better precisioncan be explained in terms of the robust properties of thealgorithmand the absence of intra- and interuser variabilitiesMoreover human registrationsweremade under the pressure
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of Biomedical Imaging 11
0
20
40
60
80
100
600 650 700 750 800 850
PlannedClinical
AutoReference
Dose (cGy)
Volu
me (
)
Figure 12 DVHs for a boost portion The planned dose was scaledto four fractions
of clinical time constraints that can hasten decisions and leadto suboptimal results
In dosimetric comparisons for the prostate automaticmapping showed less degradation in the shoulder regionof DVHs for 50 of patients in this study In the other50 degradation was no worse than the clinical protocolThe absence of large differences in dose-volume metrics isattributed to prostate margins that were relatively insensitiveto variations in isocenter mapping on the order of a few mm
The clinical significance of the observed dosimetricimprovements was not addressed but appears to be modestfor the patients in this study This conclusion howeverdepends on the prostate margin and dose fractionationscheme as suggested by Figure 12 In particular dosimetricimprovements might be significant for less forgiving formsof treatment delivery such as stereotactic body radiotherapyAlso the finding that accurate pCT and tCT image regis-tration does not fully compensate for geometric variabilitysupports conclusions of other studies [2 3] that full compen-sation for patient-specific geometric changes requires off-lineadaptive planning or online reoptimization
The overall conclusion is that the automatic algorithmrobustly maps the planned isocenter to a position close tothe correct location in a tCT and thus is well suited to aug-ment human judgment in the clinical setting Furthermorethe algorithm offers the potential for reducing registrationoutliers During the workflow for mapping the isocenterall of the essential image processing steps for calculation ofdelivered dose and mapping the delivered dose to planningspace are performed
Conflict of Interests
Edward Chaney is an employee of Morphormics Inc andPrincipal Investigator of NIH Grant no R44 CA141941 that
supported the research reported in this paper Mark Foskeyis an employee of Morphormics Inc Andrea Kress and AnQin were partially supported under subcontracts funded byNIHGrant no R44 CA141941The remaining authors declareno conflict of interests
Acknowledgment
The research reported in this paper was supported by theNational Cancer Institute of the National Institutes of Healthunder Award no R44 CA141941 The content is solely theresponsibility of the authors and does not necessarily repre-sent the official views of the National Institutes of Health
References
[1] W Y Song B Schaly G Bauman J J Battista and J vanDyk ldquoEvaluation of image-guided radiation therapy (IGRT)technologies and their impact on the outcomes of hypofrac-tionated prostate cancer treatments a radiobiologic analysisrdquoInternational Journal of Radiation Oncology Biology Physicsvol 64 no 1 pp 289ndash300 2006
[2] D Yan D Lockman D Brabbins L Tyburski and AMartinezldquoAn off-line strategy for constructing a patient-specific planningtarget volume in adaptive treatment process for prostate cancerrdquoInternational Journal of Radiation Oncology Biology Physics vol48 no 1 pp 289ndash302 2000
[3] D Schulze J Liang D Yan and T Zhang ldquoComparison ofvarious online IGRT strategies the benefits of online treatmentplan re-optimizationrdquo Radiotherapy and Oncology vol 90 no3 pp 367ndash376 2009
[4] P Jannin J M Fitzpatrick D J Hawkes X Pennec R Shahidiand M W Vannier ldquoValidation of medical image processing inimage-guided therapyrdquo IEEE Transactions on Medical Imagingvol 21 no 12 pp 1445ndash1449 2002
[5] J R Wong Z Gao M Uematsu et al ldquoInterfractionalprostate shifts review of 1870 computed tomography (CT) scansobtained during image-guided radiotherapy using CT-on-railsfor the treatment of prostate cancerrdquo International Journal ofRadiation Oncology Biology Physics vol 72 no 5 pp 1396ndash1401 2008
[6] E G A Aird and J Conway ldquoCT simulation for radiotherapytreatment planningrdquo British Journal of Radiology vol 75 no900 pp 937ndash949 2002
[7] S Sailer E L Chaney J G Rosenman G W Sherouse andJ E Tepper ldquoThree dimensional treatment planning at theUniversity of North Carolina at Chapel Hillrdquo Seminars inRadiation Oncology vol 2 pp 267ndash273 1992
[8] S X Chang T J Cullip J G Rosenman P H Halvorsenand J E Tepper ldquoDose optimization via index-dose gradientminimizationrdquo Medical Physics vol 29 no 6 pp 1130ndash11462002
[9] S M Pizer P T Fletcher S Joshi et al ldquoA method and softwarefor segmentation of anatomic object ensembles by deformablem-repsrdquoMedical Physics vol 32 no 5 pp 1335ndash1345 2005
[10] S M Pizer R E Broadhurst J Y Jeong et al ldquoIntra-patient anatomic statistical models for adaptive radiotherapyrdquoin Proceedings of the Medical Image Computing and Computer-Assisted InterventionWorkshop (MICCAI rsquo06) A Frangi and HDelingette Eds pp 43ndash46 Copenhagen Denmark October2006 From Statistical Atlases to Personalized Models Under-standing Complex Diseases in Populations and Individuals
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
12 International Journal of Biomedical Imaging
[11] D Merck G Tracton R Saboo et al ldquoTraining models ofanatomic shape variabilityrdquo Medical Physics vol 35 no 8 pp3584ndash3596 2008
[12] L E Court and L Dong ldquoAutomatic registration of theprostate for computed-tomography-guided radiotherapyrdquoMed-ical Physics vol 30 no 10 pp 2750ndash2757 2003
[13] M Smitsmans J Wolthaus X Artignan et al ldquoAutomaticlocalization of the prostate for on-line or off-line image-guidedradiotherapyrdquo International Journal of Radiation Oncology Biol-ogy Physics vol 60 no 2 pp 623ndash635 2004
[14] F Maes D Vandermeulen and P Suetens ldquoComparativeevaluation of multiresolution optimization strategies for mul-timodality image registration by maximization of mutual infor-mationrdquoMedical Image Analysis vol 3 no 4 pp 373ndash386 1999
[15] K Siddiqi and S Pizer Eds Medial Representations Mathe-matics Algorithms and Applications vol 37 chapter 8 SpringerBerlin Germany 2008
[16] M J Murphy F J Salguero J V Siebers D Staub and CVaman ldquoA method to estimate the effect of deformable imageregistration uncertainties on daily dose mappingrdquo MedicalPhysics vol 39 no 2 pp 573ndash580 2012
[17] R E Broadhurst J Stough S M Pizer and E L ChaneyldquoA statistical appearance model based on intensity quantilesrdquoin Proceedings of the 3rd IEEE International Symposium onBiomedical Imaging pp 422ndash425 April 2006
[18] S Frantz K Rohr andH Stiehl ldquoLocalization of 3D anatomicalpoint landmarks in 3D tomographic images using deformablemodelsMedical image computing and computer-assisted inter-ventionrdquo in Medical Image Computing and Computer-AssistedIntervention vol 1935 of Lecture Notes in Computer Science pp492ndash501 2000
[19] A Niemierko and M Goitein ldquoThe influence of the size ofthe grid used for dose calculation on the accuracy of doseestimationrdquoMedical Physics vol 16 no 2 pp 239ndash247 1989
[20] J F Dempsey H E Romeijn J G Li D A Low and J RPalta ldquoA Fourier analysis of the dose grid resolution requiredfor accurate IMRT fluence map optimizationrdquoMedical Physicsvol 32 no 2 pp 380ndash388 2005
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of
International Journal of
AerospaceEngineeringHindawi Publishing Corporationhttpwwwhindawicom Volume 2014
RoboticsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Active and Passive Electronic Components
Control Scienceand Engineering
Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
International Journal of
RotatingMachinery
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporation httpwwwhindawicom
Journal ofEngineeringVolume 2014
Submit your manuscripts athttpwwwhindawicom
VLSI Design
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Shock and Vibration
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Civil EngineeringAdvances in
Acoustics and VibrationAdvances in
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Electrical and Computer Engineering
Journal of
Advances inOptoElectronics
Hindawi Publishing Corporation httpwwwhindawicom
Volume 2014
The Scientific World JournalHindawi Publishing Corporation httpwwwhindawicom Volume 2014
SensorsJournal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Modelling amp Simulation in EngineeringHindawi Publishing Corporation httpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Chemical EngineeringInternational Journal of Antennas and
Propagation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
Navigation and Observation
International Journal of
Hindawi Publishing Corporationhttpwwwhindawicom Volume 2014
DistributedSensor Networks
International Journal of