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Delivery and Verification
Lutters, SRO 2011 PSI, 24.10.2011
Our goal today?
How do you define DELIVERY?
How do you define VERIFICATION?
Good DELIVERY
..
..
Good VERIFICATION
….….
Our goal today?
DELIVERY and VERIFICATION depend on
1. Mechanical properties
2. Particles physical properties
3. Mathematical models
4. Work flow/System integration
5. Patient anatomy and biology
6. Staff training and education
7. User/Patient acceptance
8. Resources, Cost, Reimbursement
9. Error free and safe to use!
Figure 2.5 (a) The Seed-Selectron with the (b) double cassette for the 125I sources
and the spacers. (Courtesy Nucletron)
Brachy seed therapy
Figure 2.10 (a) The Guidant Galileo (TM) Afterloader is using a 32P-wire source with
stepping source technology. A touch screen allows to enter the treatment parameters.
This image illustrates a possible calibration procedure with the delivery catheter inserted
into a well type chamber. (b) The 90Sr source train of the Novoste BetaCath(TM) device
is moved into the delivery catheter by using a hydraulic mechanism. During storage and
transportation the device is located in a lead storage box.
Brachy afterloader therapy
intravascular
Fig. 6. (a) Digital subtraction angiography (DSA)
of stenotic (50% luminal reduction) lesions of
left femoro-popliteal artery with normal
segment in between.
(b) DSA of proximal PTA balloon position (4 cm
length/5 mm diameter) indicating a 45 mm IL.
(c) DSA of distal PTA balloon position (4 cm
length/5 mm diameter). This second balloon
position is overlapping the proximal PTA
position expanding the IL to 75 mm.
(d) X-Ray veri®cation of 7F PARIS delivery
catheter showing the 105 mm ASL resulting in
a 100 mm RIL. Provided in co-operation with
Professor Erich Minar, MD, Division of
Angiology, Department of Internal Medicine II,
University Hospital Vienna, Vienna, Austria.
Brachytherapy
Fig. 3. (a) Cross-sectional
image of a coronary artery
from IVUS. Source,
IVUS probe and EEL are
shown. The RLDi, the isodose
lines indicating the
RLDo and the RDD, the RLDP
and the RDDP as determined
based on
angiographic ® findings are
superimposed onto the IVUS
image.
Brachytherapy
Figure 2.4 (a) The Nucletron Selectron LDR
afterloader for 137Cs pellet sources in clinical
operation
(afterloader inside the room, control unit
outside the room), and (b) the mechanism of
the source and
dummy-source selection of the device.
(Courtesy Nucletron)
Brachytherapy
Figure 2.7 Modern afterloading machines for
HDR techniques: (a) the MicroSelectron HDR
(Courtesy Nucletron), and (b) the curietronmultisource HDR (Courtesy BEBIG),
Brachytherapy
Figure 2.9 The guiding system for the check cable and the source cable of the
Nucletron MicroSelectron HDR device. In the off-position, the source is located in the
center of the tungsten safe. From there, the source can be transported through the
indexer ring to the source transfer tubes (not shown). (Courtesy Nucletron)
Brachytherapy
Figure 2.11 (a) A double C-arm fluoroscopic system integrated into the operating
theatre equipment, making the direct transfer of images to a treatment planning
system possible. (b) Images of a head-and neck implant. Due to the relatively high
cost of such integrated brachytherapy units, these systems have not found wide
distribution in the departments. (Courtesy Nucletron).
Brachytherapy
Fig. 7. Position of a library applicator (in the middle) in the transversal (left) and
sagittal (right) plane.
Brachytherapy
Figure 3.4 A Standard Imaging well type
ionisation chamber. Dedicated inserts can be
used for calibration of specified source types
at well-defined source positions. (Photograph
provided with courtesy by Varian)
The “Krieger” phantom (DGMP 1999a)
connected to a Varian afterloading unit. For
each phantom design (distance between
sources and ion chamber, size and material of
the phantom) and source type the correction
factor for lack of full scatter needs to be
determined separately.
Brachytherapy
Figure 6.2 Check ruler and marker wire to
determine the programmed position of the
source in a stepping HDR or PDR source
afterloader. (Courtesy Varian), (b) Set of
orthogonal images taken on a C-arm X-ray unit
of a uterine tube and two shielded ovoids
showing the position of the shields inside the
ovoids. (Courtesy Varian)
Brachytherapy
Figure 6.3 (a) Autoradiograph of the source positions programmed with an HDR
afterloader with 6 catheters placed directly on the surface of a verification film
(Kodak XV film). (b) The “Baltas” phantom, designed for geometry checks in
brachytherapy.
Brachytherapy
IORT (Novac7)
Novac7 and MOBETRON: The first scope of
application was in breast cancer, at that time the
big innovation was the boost radiation or in a
single dose and at the same time as the
resection in the operating room (ELIOT).
Intraoperative radiotherapy (IORT) using PeC (Carl-Zeiss) system is a method of
delivering conformal radiotherapy to the tumor region. The small tumors (2-4 cm
diameter) of the brain and breast cancer are precisely excised and irradiated using
special IORT applicators and verified by onsite pathologists providing frozen
section pathology input.
IORT (IntraBeam)
IORT (IntraBeam)
MammoSiteMammoSite-catheter is placed in the cavity after surgery and filled with saline solution.
Two times a day for five days a HDR unit moves the source into the balloon.
MammoSite
Also MammoSite-treatment can be planned with modern TPS. The optimization of dose distribution, adaption to target volume is limited.
IORT Comparison
IORTProblems: Dosimetry (6 and 18MeV electrons, angled and straight)Either Linac in surgery theatre (shielding!) ordesinfection of Linac bunker
X-Ray EBRT
1. Energy 20-80kV (superficial) or 80-300kV (ortovoltage)
2. Dose distribution fixed by applicator shape and size (Individual cut-outs)
3. Depth dose depends on tube length
1. Difficult targeting and dosimetry
2. Low cost and complexity
3. Used for benign tumors, inflammatory diseases
EBRT devices with radioactive sources
Gammaknife
An Elekta Leksell gamma knife used in radiosurgery of the head
Single day treatment, stereotactic ring fixed in scull, precise
Boron Neutron Capture
Boron Neutron Capture
Accelerator based systems
Depth dose comparison (focus to superficial tumors i.e. breast cancer)
What is the best modality?
C-Arm Linac head
C-Arm Linac add-ons
EPID
Treatment Table
External coordinate system (laser, camera)
Fluoroscopy & cone-beam CT system (kV, MV)
Record and verify
Linac
Construction of the head of Elekta Precise®
accelerator
[1].
Figure
Accelerating structure of Elekta Precise® [2].
C-Arm Linac
MLC design
MLC design
Flattened beam vs. IMRT
Reasons?
Optimal Plan? Optimal delivery?
Who does better?
•Linac mechanics
•Beam production
•Record and Verify
•Imaging
Or is TPS or R&V insufficient?
Movement of Linac and Table
HD250 (SIEMENS) tries to simulate an 250 leaf MLC by moving collimator head, MLC and table (not supported by TPS!)
Tomotherapy
Complete system: CT, TPS, rotational IMRT with moving table and CBCT in one device.
What are the limitations?
Tomotherapy
Delivering techniques
Flattened vs. unflattened Beams.
IMRTsMLCdMLCVMATRotational IMRT flattening filter free
Differences?……
Imaging
What is the goal, what do we need to see?
…
CT on rails
Pro: real diagnostic image quality
Con: no absolute coordinate origin
Cyberknife
Robotic system (Linac arm and table)
Integrated verification and motion management system
Field size fixed by cone diameter
Dose is build up by many spots
Electron IMRT (MERT)
Radiotherapy and Oncology Volume 100, Issue 2, August 2011, Pages 253-258 Comparison of modulated electron radiotherapy to conventional electron boost irradiation and volumetric modulated photon arc therapy for treatment of tumour bed boost in breast cancerAndrew Alexander a, et al. McGill University, Montreal, Quebec, CanadaAbstract
Background and purposeTo compare few leaf electron collimator (FLEC)-based modulated electron radiotherapy (MERT) to conventional direct electron (DE) and volumetric modulated photon arc therapy (VMAT) for the treatment of tumour bed boost in breast cancer.Materials and methodsFourteen patients with breast cancer treated by lumpectomy and requiring post-operative whole breast radiotherapy with tumour bed boost were planned retrospectively using conventional DE, VMAT and FLEC-based MERT. The planning goal was to deliver 10 Gy to at least 95% of the tumourbed volume. Dosimetry parameters for all techniques were compared.ResultsDose evaluation volume (DEV) coverage and homogeneity were best for MERT (D98 = 9.77 Gy, D2 = 11.03 Gy) followed by VMAT (D98 = 9.56 Gy, D2 = 11.07 Gy) and DE (D98 = 9.81 Gy, D2 = 11.52 Gy). Relative to the DE plans, the MERT plans predicted a reduction of 35% in mean breast dose (p< 0.05), 54% in mean lung dose (p < 0.05) and 46% in mean body dose (p < 0.05). Relative to the VMAT plans, the MERT plans predicted a reduction of 24%, 36% and 39% in mean breast dose, heart dose and body dose, respectively (p < 0.05).ConclusionsMERT plans were a considerable improvement in dosim etry over DE boost plans. There was a dosimetric advantage in using MERT over VMAT for inc reased DEV conformity and low-dose sparing of healthy tissue including the integral do se; however, the cost is often an increase in the ipsilateral lung high-dose volume.
EMLC
The EMLC consists of 30 brass leaf pairs with the bottom edge located 16 cm above the isocenter. The resulting maximum field size at 100 cm isocenter is 21.4 cm x 21.4 cm. All leaves can be moved up to a fourth of the maximum field size beyond the central field axis (leaf overtravel).
In comparison with the standard applicator from 6 to 14 MeV, the only differences in dose distribution are the greater beam penumbra of 0.7 to 0.3 cm and the larger build-up effect in the depth-dose curves quantified by the lower surface dose of 3 to 4%. Radiation leakage of the EMLC at 14 MeV amounts to 1.5 to 2.5% relative dose, which could be effectively reduced up to the dose contribution from photon contamination of the electron beam due to our tongue-and-groove leaf design. The total weight of the EMLC is 23 kg. “Elekta Research Prize” for the development. The ESTRO honoured this
development with the “Jack Fowler-University of Wisconsin Award”. Images T.Gauer Diss. Uni Hamburg
Heavy Particle Therapy
J Radiat Res (Tokyo). 2010;51(4):365-83. Recent advances in the biology of heavy-ion cancer therapy. Hamada N, et al Radiation Safety Research Center,, Komae, Tokyo, Japan. t
Superb biological effectiveness and dose conformity represent a rationale for heavy-ion therapy,
which has thus far achieved good cancer controllability while sparing critical normal organs.
Immediately after irradiation, heavy ions produce dense ionization along their trajectories, cause
irreparable clustered DNA damage, and alter cellular ultrastructure. These ions, as a consequence,
inactivate cells more effectively with less cell-cy cle and oxygen dependence than
conventional photons. The modes of heavy ion-induced cell death/inactivation include apoptosis,
necrosis, autophagy, premature senescence, accelerated differentiation, delayed reproductive death
of progeny cells, and bystander cell death. This paper briefly reviews the current knowledge of the
biological aspects of heavy-ion therapy, with emphasis on the authors' recent findings. The topics
include (i) repair mechanisms of heavy ion-induced DNA damage, (ii) superior effects of heavy ions
on radioresistant tumor cells (intratumor quiescent cell population, TP53-mutated and BCL2-
overexpressing tumors), (iii) novel capacity of heavy ions in suppressing cancer metastasis and
neoangiogenesis, and (iv) potential of heavy ions to induce secondary (especially breast) cancer.
Pion Therapy
Pions belong to a group of short-lived subatomic particles called mesons. They
are the lightest of the mesons, having about one seventh the mass of protons
or neutrons. Some are electrically neutral, while others carry a single positive or
negative charge . Pions are not normally found in the free state in nature: when
a nucleus is struck by a proton having a certain energy, pions are ejected from
the nucleus. Beams of charged pions can be guided, bent or focused by
magnetic fields, just as light beams are controlled by prisms or lenses
Applikation Protonen
Proton
Proton Gantry
Photon Gantry
Proton facility
Heavy Ion
One room proton facilities
BIG ROOMS! Cheaper? Acceleration WIP. No Gantry?.
Tomotherapy Proton facility
Conventional protons are delivered with only a few fields. Photon Tomography has greater high dose conformity but there is less integral dose with protons.
Dielectric wall accelerator• DWA is a multistage inductive accelerator underdevelopment at Lawrence Livermore National Lab.• Acceleration gradient of 100 MV/m possible.• 200 MeV protons in 2 meters.• Beam energy, intensity and spot size variable pulse-topulse.• IMPT can be achieved with spot scanning or distal edge tracking through limited arcs.
The method has been implemented clinically at GSI Darmstadt. The picture shows the
treatment of a patient with a skull base tumour at the heavy ion treatment facility at GSI
Darmstadt. For a precise positioning the head of the patient is fixed by means of an
individual mask. The gamma quanta generated by the positron annihilation are marked
in red. Above and below the patient the detectors of the positron emission tomograph
are mounted.
Heavy Ion
Proton delivery technique
Scanning
Scatter
Passive Scattering
• Range Shifter Wheel
um Bragg-Peakauszuziehen (entlang der Tiefenachse)
• Scatterer um Strahl aufzustreuen (seitlich zur Tiefenachse)
• Filter
• Kompensatoren um der Geometrie des Tumors gerecht zu werden
Active Scanning
Lomax, Pedroni, PSI Villigen
Eye tumors
Bilder Hug E, PSI Villingen
Comparison Photons Protons
Tumor sizeMotion inter- and intra-fractionSpecific uncertaintiesDose rate (treatment time)Verification....
Biology enhanced treatments
Always in addition radio therapy !
Temperatures 39-43 degree Celsius in target region
Microwave Hyperthermia Nano particles as carriers Nano particles as heat generatorsHigh Focused Ultrasound
Advantage: NO extra long term side effects
Superficial hyperthermia● Range ~ 1 – 3 cm
water bolus
0
3
6
9
12
151 4 7 10 13
Z [°C]
X [cm]
Y [cm]
Spiral-Applikator-8
42-42.5
41.5-42
41-41.5
40.5-41
40-40.5
39.5-40
39-39.5
38.5-39
38-38.5
37.5-38
37-37.5
36.5-37
36-36.5
35.5-36
35-35.5
Superficial-HT: Spiral applicators
dimensions (5-24cm)water-bolus-system8/24 channelindividually controllableadaption to the heat distribution
Deep Hyperthermia
8 antennas
•software for a 2D-field control
THT planning
QA–tool: Lamp phantom
Effect of operating frequencySigma-60
0
10
20
30
40
50
70 80 90 100 110 120 130
frequency MHz
% re
flect
ion
76 MHz 92 MHz 125 MHz
THT
Diversity of
nanoparticles used in
drug delivery strategies.
Nanoparticulate
formulations can be
tailored based on the
required drug to be
encapsulated/carried.
While hydrophobic
molecules can be
incorporated inside the
core of the nanoparticles,
hydrophilic molecules
can be carried more
readily within an aqueous
core protected by a
polymeric or lipidic shell.
Nano particles
Nano particles (MagForce)
NanoTherm® therapy is a new approach for the local treatment of solid tumors. The principle
of the method is the direct introduction of magnetic nanoparticles into a tumor and their
subsequent heating in an alternating magnetic field. The water soluble nanoparticles are
extremely small (approximately 15 nanometers in diameter), and contain an iron oxide core
with an aminosaline coating. The particles are activated by a magnetic field that changes its
polarity 100,000 times per second, and heat is produced.
Depending on the duration of treatment and the achieved intratumoral temperatures, the
tumor cells are either directly destroyed (thermal ablation) or sensitized for concomitant
chemo or radiotherapy (hyperthermia).
With this new procedure, it is possible to combat the tumor from the inside out, thereby
sparing surrounding health tissue. The nanoparticles remain in place at the treatment area,
allowing for repeated treatments and the integration of multimodal therapy concepts.
HIFU
The in the MRT integrated ultrasound unit
sends focussed impulses to the myomas.
Verification Imaging
What is the goal?
Treatment chain verification !
• http://www.astro.org/Meetings/ConferencesAndSymposia/IGRTSymposium/ScientificProg
ram/documents/Amies.pdf
Fig. 5. Dose calculation on patient treated for recurrent naso-pharyngeal carcinoma with intensity-modulated radiotherapy. No weight loss or anatomy deformation observed between CT and megavoltage cone-beam CT (MVCBCT).(Above) Isodose lines at treatment isocenter planes on conventional CT and MVCBCT.(Below) Good qualitative agree-ment observed with dose–volume histograms obtained from dose calculations performed using CT (solid lines) and MVCBCT (dashed lines).
I. J. Radiation Oncology ● Biology ● Physics Volume 67, Number 4, 2007
Adaptive RT
Conventional CT reconstruction 2 mm (IMRT pelvis, H&N,)
CT with Gating to determine the security margindepending on the movement of the tumour.IMRT breast, 3D conformal lung>
in the future IMRT lung
security margin depending on the movement of the tumour
Bildaufnahme
Verification fluence with FPP + 3D Delta 4 detector
With original Gantry angle
FPP Fluenze Verifikation
Multi point 3D absolute dose check
With original Gantry angleTable effect
+
=?
TPS Dose
Delta 4 Dose (measured)
=?
Dose verification with FPP + MU–Future
With original Gantry angle
Multi point MU checkData transfer check
MU CALCULATOR DIAMOND
+
=?
FPP Fluenze Verifikation
Patient-specific QASetup Verification
• Standard
� Orthogonal portal vs. DRR
- (FPP, film, CR)
� Verification Isocenter
� Field shape/perture (port during)
� preferred
� MVCB
� Isocenter verification
� Tumor (markers), OAR, outline change monitoring
Dosisaspekt bei MVCB CT
We can calculate the applied dose. In the IMRT optimization we can even consider the dose from the MVCB-CT (Pinnacle 7.6 c, KonRad 2.2.)
KonRad 2.2 Plannung Karin Markl, Siemens
Pinnacle7.6 c Planung Shaka Khan, KSA
DOSE CALCULATION
DOSE COMPENSATION
Lutters IMRT clinical implementation at KSA, Heidelberg IMRT IGRT School ,2007
Pre-Treatment 3D Dose verification In-vivo 3D Dose verification Nijsten et al. MAASTRO Physics Abstract
Pre -tretment
In vivo 3D dose reconstruction in MVCB CT
IMRT chain control
Positioning and immobilization
Image acquisition
Structure segmentation
Treatment planning and evaluation
File transfer and management
Plan validation
Setup verification
IMRT treatment delivery and verification Ezzell et al, 2002
Patient specific QASetup verification
• Standard� Orthogonal portal vs. DRR - (FPP, film, CR)� Isocenter verification� Field shape/aperture (port
during)
� Preferable� MVCB/kV CBCT/CT on rails � vs. CT� Isocenter verification� Tumor (markers), OAR, outline
change monitoring
Consider protocols for setup correction e. g. NAL
Pre-Treatment 3D Dose verification In-vivo 3D Dose verification Nijsten et al. MAASTRO Physics Abstract
Pre -tretment
In vivo 3D dose reconstruction in MVCB CT
Exit dosimetry, EPID in vivo
Differences between predicted and measured portal dose during breast treatment ∆D =3% , Δr=5 mm
W. J. C. van Elmpt et al., Medical Physics, Volume 32, Issue 9, pp. 2805-2818, September 2005.
Non-ionising verification
Calypso: Tumor GPS
Vision RT: Surface detection
Tracks the 3D surface of a patient in real time without the need to apply external markers or any other physical device to the patient.
MOSAIC xxx: Accessory registration
New design for motion and verification adaption
Adaptive RT and Dose summation
Most common evaluation parameters:
� Gamma index (Law et al. 1998), see Figure� DTA (Distance To Agreement)the distance between a measured data point and the nearest point in the calculated dose distribution that exhibits the same dose.
� Dose difference� Isodose overlay
Other : NAT =Normalized Agreement Test(Childress et al.2004) , Gradient analysis (Moran et al., 2005)
Patient specific QAEvaluation
Figure Gamma concept. Depuydt, 2002
Common gamma criteria: ∆D = 3 - 4% ; ∆d =2 - 3 mm Gamma passed when ≤ 1other criteria % points <1 , < 1.5, <2
Statistical analysis of the results helps to set up protocols with criteria of acceptability
DGRT: it’s the dose that matters
Volumetric-modulated arc therapy (VMAT) entails rap id execution of a sequence of control points each defi ning multileaf collimator (MLC) shape, MLC segment dose, and a gantry-angle window across which each shape sweeps dynamically.
Adaptive radiotherapy ART
Dose-guided radiotherapy
MVCBCT and DGRT
Every new machine enables us to do a better treatment !
Consider a prostate, breast and lung treatment
Which machine do you choose?• Tomotherapy• Linac• Cyberknife• Protons
• Which technique do you choose?• IMRT/IMPT, IMAT, etc.• Gating• Stereotaxy
Machines deliver planned dose distributions !
Which TPS (algorithm) do you choose?• Stereotaxy calculation • Pencil beam• Convolution/collapsed cone• Monte Carlo
Which verification system do you choose?• Film/CR• EPID• Cone beam (kV or MV) or InRoom CT• Soft Tissue or Markers or Bony Landmark
Congratulations: You chose the best system
Accuracy of • modality• dose distribution• dose calculation• verification image qualityis simply the best
BUT: Did you think about • the patient and• his physician ?Do they fit into the precision of delivery and veri fication?
How precise is the patient?
Setup errors consist out of• Systematic errors• Random errors• Motion errors
Systematic errors are…..
Random errors are …
Motion errors are ……
Geometric Uncertainties in Radiotherapy; Defining the Planning Target Volume, British Institute of Radiology (Januar
2003) ISBN-10: 0905749537 ISBN-13: 978-0905749532
How precise is the patient?
Difficult to determine in advance for an individual patient.
ICRU52 and 60 define the target and organ at risk v olumes. They introduce a margin concept for unpredictable e rrors.
Solution: population based margin recipes (Marcel v . Herk)http://www.aapm.org/meetings/amos2/pdf/35-9817-23186-884.pdf
How precise is the physician
• Inter-observer variability• Intra-observer variability• Use of multimodality imaging• Understanding MRI/PET• Management of motion (artifacts)• Tumor staging • Tumor delineation
What is the QA for the physicians work?
Solution: Get a colleague to review every contour, dose plan, verification image every time.
http://www.rcr.ac.uk/docs/oncology/pdf/BFCO(08)5_On_target.pdf
Total uncertainty
• Dosimetry• Calculation • Delivery• Verification• Delineation• Set up • Motion
What is the biggest error, where is it easiest to i mprove?
->Intra- and inter-observer variability in tumor del ineation!CF Njeh, Tumor delineation: The weakest link in the search f or accuracy in radiotherapy ; Journal of Medical
Physics; Review article, 2008, Volume : 33, Issue : 4, Page : 136--140
Greetings to PSI neutron imaging