Upload
others
View
6
Download
0
Embed Size (px)
Citation preview
Bern University of Applied Science | HuCE-optoLabt
Real Time Process Control with Optical Coherence Tomography
▶ HUCE, OPTOLAB
16th of June 2016,
Ch. Meier
Bern University of Applied Science | HuCE-optoLab
▶ Short introduction to OCT Systems ▶ Resolution and NA, ▶ SD OCT and SS OCT, Scanning and Full Field Systems
▶ Examples of Real Time Process Control using OCT
▶ Braucht mindestens 30 min. Lasik Film ist aus der Präsentation gelöscht
Overview
Bern University of Applied Science | HuCE-optoLab
Introduction and Theory
Bern University of Applied Science | HuCE-optoLab
▶ Comparable with ultrasonic tomography▶ measuring the time delay of
back-scattered or back-reflected light▶ Too short time delays for direct
measurements▶ interferometric measurements
OCT: Basic principle
A-scan, spatial domain
B-scan
0 100 200 300 400 5000
2000
4000
6000
0
Bern University of Applied Science | HuCE-optoLab
▶ Cross sectional images obtained by scanning in x and y direction
▶ A-scan, B-scan, C-scan
3D Imaging by lateral scanning
Bern University of Applied Science | HuCE-optoLab
Diagnostic window
0.7 0.8 0.9 1.0 1.1 1.2 1.3 1.4 1.5 >1.6
Silicon InGaAs PbS or PbSe
OphthalmicRetina, anterior segment
Cardiovascular,Dermatology, other tissue
NDT, QA
Laser
Apll.
Det.
Bern University of Applied Science | HuCE-optoLab
Michelson Interferometer setup with moving reference mirror
The signal envelope represent the scattering or reflectivity depth profile
Time Domain OCT
Bern University of Applied Science | HuCE-optoLab
Source S(λ)
zz0
z1
SpectrometerSpectrometer
FD OCT, Spectrometer based
Bern University of Applied Science | HuCE-optoLab
Source S(λ)
z
sample
z0
z1
SpectrometerSpectrometer
Interferences due tooptical path difference
Frequency in k‐space is proportional to OPD
Scattering or reflectivity depth profile is obtained by a Fouriertransformation
FD OCT, Spectrometer based
Bern University of Applied Science | HuCE-optoLab
200 400 600 800 1000 1200 1400 1600 1800 20000
500
1000
1500
2000
2500
3000
3500
4000
Inte
nsity
a.u
.Swept Source OCT
0
Detector
Bern University of Applied Science | HuCE-optoLab
-50 0 500
0.2
0.4
0.6
0.8
1
Distance in um
Inte
nsity
in a
.u.
0.8 0.82 0.84 0.86 0.88 0.90
0.2
0.4
0.6
0.8
1
Wavelengh in um
Inte
nsity
in a
.u.
▶ General signal in Frequency Domain
▶ General signal in Frequency Domain
▶ Gaussian source spectrum -> Gaussian PSF
▶ PSF = axial resolution = Coherence Length
Axial Resolution
-50 0 500
0.2
0.4
0.6
0.8
1
Distance in um
Inte
nsity
in a
.u.
0.8 0.82 0.84 0.86 0.88 0.90
0.2
0.4
0.6
0.8
1
Wavelengh in um
Inte
nsity
in a
.u.
-50 0 500
0.2
0.4
0.6
0.8
1
Distance in um
Inte
nsity
in a
.u.
0.8 0.82 0.84 0.86 0.88 0.90
0.2
0.4
0.6
0.8
1
Wavelengh in um
Inte
nsity
in a
.u.
Bern University of Applied Science | HuCE-optoLab
Lateral resolution Axial resolution
Confocal Microscope
OCT
Coherence gate
Resolution
Bern University of Applied Science | HuCE-optoLab 13
FD OCT
TD OCT Source S(λ)
Cam
Swept Source
Cam
z
SLED
z0
SS
Detector
z0
Full Field OCT Scanning OCT
SLED
z0
Detector
Bern University of Applied Science | HuCE-optoLab
Scanning versus Full Field OCT
cam
Scattering media
SM fiber
Confocal gate
Coherence gate
Coherence gate
Bern University of Applied Science | HuCE-optoLab
▶ A-scan rate
▶ 512 lines/frame, 512 frames
Acquisition Time
A_Scan rate/kHz B-scan rate/ Hz
C-scan rate/ Hz
100 195 0.38
200 390 0.76
850 1660 3.24
Camera Line rate /kHz Swept Source Rate /kHz
AVIIVA 100 Santec 50 - 100
Basler 140 Axsun, Insight,Thorlabs
100- 200
Fraunhofer, AIT 600 OCTLight 850
OptoRes 1500
Bern University of Applied Science | HuCE-optoLab
Examples of Real Time Process Control
Bern University of Applied Science | HuCE-optoLab
▶ Phase–Sensitive Parallel Optical Coherence Tomography
▶ Number of pixels: 300 x 300▶ Smart pixels (demodulation) ▶ Frame rate up to 10^6/s▶ C-scan rate 3-6 Hz
(1mm depth)
Full Field OCT
Bern University of Applied Science | HuCE-optoLab
▶ Solder Bumps
Topographic measuremenents
Bern University of Applied Science | HuCE-optoLab
Layer thickness measurement
19
Bern University of Applied Science | HuCE-optoLab
Layer thickness measurement
20
Bern University of Applied Science | HuCE-optoLab
Schichtdickenmessung in Schläuchen
21
Bern University of Applied Science | HuCE-optoLab
Optimized Laser Head for Contact-Free Osteotomy with real time Depth Control
Advanced Osteotomy Tools
▶ Robot for bone cutting▶ Clean cuts, better healing
Bern University of Applied Science | HuCE-optoLab
Measurement of cutting depth
Advanced Osteotomy Tools▶ After each laser-shot one
B-scan for depth measurement
Bern University of Applied Science | HuCE-optoLab
Ultra-high Resolution OCT Monitoring for Dosimetry Control during Selective Retina Laser Treatment
Sourc
e: T
opco
n
▶ Coagulation of RPE, photoreceptor cells, choroid▶ Introduced tissue damage is irreversible▶ Excessive tissue damage for RPE-linked pathologies[1]
[1] Brinkmann R, and Birngruber R, Medizinische Physik 2007; 17:6‐22
Bern University of Applied Science | HuCE-optoLab
Selective Retina Therapy (SRT)
Retina: en‐face view. Treatment sites (white) at different power levels and treatment plan
▶ Sub-threshold laser treatment
▶ Tissue damage remains limited to the retinal pigment epithelium (RPE)
▶ Introduced retinal lesions remain ophthalmoscopically barely visible or invisible
▶ Dynamic changes in tissue detected by time-resolved OCT providereal-time feedback for laser dosimetry
Bern University of Applied Science | HuCE-optoLab
▶ Effects originate in RPE / Bruch’s membrane complex and expand to inner retina
▶ Signals linked to thermal expansion, thermal vibration and changes in tissue scattering
▶ Axial tissue movement in the range of few μm/s up to few m/s detectable
Time-resolved OCT data
26
~ 100 mm/s
P. Steiner. PhD Thesis 2015
Bern University of Applied Science | HuCE-optoLab
Clinical SRT Studies: OCT Visibility
27P. Steiner. PhD Thesis 2015
Bern University of Applied Science | HuCE-optoLab
▶ Thermal vibrationshockwaves introduced by abrupt heating
▶ Thermal expansionlong term changes after the pulse, typical relaxation times of tens of ms
▶ Rapid dynamic changes Rearrangement of scatterers due to microbubble creation
Damage mechanisms
28P. Steiner. PhD Thesis 2015
Bern University of Applied Science | HuCE-optoLab
Real Time Optical Coherence Tomography Laser Dosimetry control during Selective Retina Therapy
Bern University of Applied Science | HuCE-optoLab
Investigation with technical samples
P. Morgenthaler Master Thesis 2016
Bern University of Applied Science | HuCE-optoLab
Seeing Surgical Laser
(CTI 12984)
▶ Surgical laser equipped with measurement and visualization system
▶ Enables planning and controlling the surgery
▶ Product launch 2014
Bern University of Applied Science | HuCE-optoLab
▶ Algorithms to extend the imaging range
▶ Surgery planning by touch screen
Challenge: Data Processing
Bern University of Applied Science | HuCE-optoLab
HuCE-optoLab
Thank you for your attention