statistical reconstruction for soft tissue imaging with...
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![Page 1: Statistical Reconstruction for Soft Tissue Imaging with ...istar.jhu.edu/pdf/Wang_Fully3D2013_vDistrib.pdf · A. Wang et al (Johns Hopkins University) . 06/18/2013 . Presented at](https://reader031.vdocuments.us/reader031/viewer/2022030501/5aadc62a7f8b9a190d8b563e/html5/thumbnails/1.jpg)
A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 1
CT CBCT
Johns Hopkins University Schools of Medicine and Engineering
Statistical Reconstruction for Soft Tissue Imaging
with Low Dose C-arm
Cone-Beam CT
Adam S. Wang,1 J. Webster Stayman,1 Yoshito Otake,1 Gerhard Kleinszig,2 Sebastian Vogt,2
A. Jay Khanna,3 Ziya L. Gokaslan,4 and Jeffrey H. Siewerdsen1
1Biomedical Engineering, Johns Hopkins University
2XP Division, Siemens Healthcare 3Orthopaedic Surgery, Johns Hopkins University
4Neurosurgery and Oncology, Johns Hopkins University
CT CBCT
Acknowledgments
The I-STAR Laboratory Imaging for Surgery, Therapy, and Radiology
www.jhu.edu/istar
Hopkins Collaborators School of Medicine
G. Gallia, D. Reh
School of Engineering R. Taylor, G. Hager, J. Prince
Siemens XP R. Graumann
Funding Support Siemens Healthcare (XP Division)
National Institutes of Health
Johns Hopkins University Schools of Medicine and Engineering
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 2
Mobile C-arm
Intraoperative C-arm CBCT High-precision surgical guidance Detection of complications OR quality assurance Challenges Higher noise, artifact than diagnostic CT Conventionally limited to high contrast (bone, contrast enhanced vessels) Need for lower dose (patient and staff) Opportunities Statistical reconstruction Extend low-dose CBCT to soft-tissue surgeries
Motivation
Faster acquisition If acquisition limited by frame/source rate Reduce patient motion
Gated acquisition Novel geometries and trajectories … Lower dose (?) (a) Lower mAs per projection: better sampling (b) Undersample: avoid electronic noise floor Impact on image quality?
Sparse Sampling in Image-
Guided Surgery
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 3
Soft Tissue Imaging Large (>10 mm), low contrast (< 100 HU) tasks Image quality assessment: Compare to FBP Emphasis on fair comparison (noise and resolution) Abdomen Anthropomorphic Abdomen Phantom Cadaver Abdomen Low-Dose CBCT Protocols 100 kVp, (15 – 120) mAs CBCT: 100 kVp, 120 mAs (3.1 mGy)† (c.f., MDCT: ~10 – 25 mGy)‡
Sparse Acquisitions Compare {100%, 50%, 25%} projections at equal dose
Overall Approach
30 cm
†Schafer et al, Med Phys 2011 ‡Sagara et al, Am J Roentgen 2010
Experimental Methods Image Acquisition Motorized orbit: angular range 178° 200 projections FOV: 15×15×15 cm3 768×768 pixels (0.6 mm isotropic voxels) PaxScan 3030+ FP detector Dual-gain mode 2×2 binning: 0.388 mm Image Reconstruction Penalized likelihood (PL) † Separable quadratic surrogates (SQS) Allows all voxels to be updated simultaneously Requires 1 forward-, 1 back-projection per iteration Ordered subsets allows speedup ~# subsets Separable footprints (SF-TT) projector‡
CUDA implementation on Nvidia GTX 680 † Erdogan and Fessler PMB 1999 ‡ Long et al IEEE TMI 2010 ‡ Wu and Fessler Fully3D 2011
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 4
Image Reconstruction Penalized likelihood (PL) † Separable quadratic surrogates (SQS) Allows all voxels to be updated simultaneously Requires 1 forward-, 1 back-projection per iteration Ordered subsets allows speedup ~# subsets Separable footprints (SF-TT) projector‡
CUDA implementation on Nvidia GTX 680
Experimental Methods Image Acquisition Motorized orbit: angular range 178° 200 projections FOV: 15×15×15 cm3 768×768 pixels (0.6 mm isotropic voxels) PaxScan 3030+ FP detector Dual-gain mode 2×2 binning: 0.388 mm
† Erdogan and Fessler PMB 1999 ‡ Long et al IEEE TMI 2010; Wu and Fessler Fully3D 2011
Voxel
Detector
Source
arg maxˆ log ( ; ) ( )L y R
Data consistency
Roughness penalty
Consider equal-dose scans, same recon time: (a) 100% P projections, 100% mA
N iterations, M ordered subsets
A·C·B·D|A·C·B·D|A·C·B·D|A·C·B·D|···
(b) 50% P projections, 200% mA 2N iterations, ½ M ordered subsets
A·C|A·C|A·C|A·C|A·C|A·C|A·C|A·C|···
(c) 25% P projections, 400% mA 4N iterations, ¼ M ordered subsets
A|A|A|A|A|A|A|A|A|A|A|A|A|A|A|A|···
Sparse Sampling
A B C D
A
C
A
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 5
0.015
0.02
0.025mm-1
-200
-100
0
100
200
300
HU CBCT: PL
Anthropomorphic Abdominal Phantom Projections fully truncated Best-fit elliptic cylinder estimated from projections - Provide support region, initialization for PL reconstruction Low contrast sphere (-80 HU, 12.7 mm diameter) 1000 HU ≈ 0.02 mm-1
C-arm FOV
Ellipse Support
Diagnostic CT
Low Contrast Target (-80 HU)
Soft-Tissue Imaging
Penalty
Difference
jk j kj k N
R w
2
jk j kj k N
R w
21 , | |2( )
| | , | |2
H
x xx
x x
3D Neighborhood
Noise-Resolution Tradeoff PL: Roughness Penalty Penalize the difference between neighboring voxels
Quadratic Penalty Tends to enforce smoothness throughout image
Huber Penalty Relatively less penalty for large pixel differences Attempts to preserve edges
Quadratic
Linear
Huber
Linear Quadratic
-δ δ
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 6
jk j kj k N
R w
3D Neighborhood
Noise-Resolution Tradeoff PL: Roughness Penalty Penalize the difference between neighboring voxels
Filtered Backprojection
Ramp filter applied with apodization window Cutoff frequency fc Fair comparison should also introduce smoothing in z-direction Use 2D apodization window that is applied in u- and v-directions of projection
u
v
fu fu fc -fc
Ramp
Apodization
fv
0.5 0.75 1 1.25 1.50
5
10
15
20
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
5
10
15
20
ESF Width (mm)
CN
R
Noise-Resolution Analysis
Tradeoff between CNR and ESF Low contrast sphere (-80 HU) Edge Spread Function (ESF) captures lower resolution with increasing regularization strength β
2
0
2erfx tx e dt
( ) erf2 2c xf x a
0 2 4 6 8 10 12-100
-80
-60
-40
-20
0
20
40
60
Distance (mm)
Attenuation (
HU
)
c σ
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 7
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
0.5 0.75 1 1.25 1.50
10
20
30
40
50
ESF Width (mm)
CN
R
Abdomen Phantom
Noise-Resolution Tradeoff 100 kVp, 60 mAs Images shown at ESF σ = 1 mm Select δ = 5 HU as balance between CNR and blocky, piecewise-constant
δ = 1 δ = 3
δ = 5
δ = 10
δ = 20 PL-Q
FBP
δ = 1 * δ = 3 δ = 5
δ = 10 δ = 20 PL-Q
FBP
20 40 60 80 100 1200
5
10
15
20
25
30
35
mAs
CN
R
15 mAs 30 mAs 60 mAs 120 mAs
FBP
PL
½ Dose
2.2× CNR
PL
FBP
Abdomen Phantom
Low Dose Comparison 100 kVp, {15, 30, 60, 120} mAs Matched resolution Low contrast ESF width σ = 1 mm PL-Huber (δ = 5 HU) vs FBP
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 8
20 40 60 80 100 1200
5
10
15
20
25
30
35
mAs
CN
R
20 40 60 80 100 1200
5
10
15
20
25
30
35
mAs
CN
R
Equal dose, resolution, recon time (PL) Same total dose: {15, 30, 60, 120} mAs Fixed ESF: σ = 1 mm P = 192 projections, N = 100, M = 32 Sparse sampling (50% P) beneficial at
ultra low dose (~40 mAs)
Sparse Sampling 100% P
50% P
25% P
100% P
Sampling
50% P
25% P
15 mAs Total Dose
30 mAs 60 mAs 120 mAs
FBP
FBP
PL
PL
100% P
50% P
25% P
15 mAs Total Dose
30 mAs 60 mAs 120 mAs
Realistic Soft Tissue Imaging Fresh cadaver (non-fixed) Apply abdomen phantom parameters for matched resolution 80 HU contrast ESF width σ = 1 mm PL-Huber (δ = 5 HU) vs FBP 100 kVp, 480 mAs used for reference images
Cadaver Abdomen
164/330351/500
224/350
0.014
0.015
0.016
0.017
0.018
0.019
0.02
0.021
0.022
0.023
0.024
164/330351/500
224/350
0.014
0.015
0.016
0.017
0.018
0.019
0.02
0.021
0.022
0.023
0.024
164/330 351/500
224/350
0.014
0.015
0.016
0.017
0.018
0.019
0.02
0.021
0.022
0.023
0.024
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 9
FBP
PL
60 mAs 30 mAs 120 mAs 15 mAs
20 40 60 80 100 1200
2
4
6
8
10
12
14
16
mAs
CN
R
1.4× CNR
½ Dose Low Dose Comparison Noise calculated from subtraction with respective reference images 100 kVp, {15, 30, 60, 120} mAs PL reduces noise, preserves high contrast structures
Cadaver Abdomen PL
FBP
Sparse Comparison Fully sampled better at higher dose 50% sparsity better at lower dose Suggests two regimes for dose reduction strategy
Cadaver Abdomen
60 mAs 30 mAs 120 mAs 15 mAs
100% P
50% P
25% P
Sampling
20 40 60 80 100 1200
2
4
6
8
10
12
14
16
mAs
CN
R
100% P
50% P
25% P
PL
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A. Wang et al (Johns Hopkins University) www.jhu.edu/istar
06/18/2013
Presented at Fully 3D Image Reconstruction in Radiology and Nuclear Medicine 2013, Lake Tahoe 10
Statistical Reconstruction Improvements in CNR by a factor ~1.4-2.2× at ½ dose for soft tissue imaging Fair comparison achieved by matching resolution w.r.t. low-contrast target
Dose Reduction Strategy Lower tube current, then go sparse Sparse advantage in overcoming electronic noise Crossover point function of imaging task, and electronic vs quantum noise levels
Advanced Modeling Scatter correction Polyenergetic spectrum Electronic noise model
Conclusion & Future Work
FBP PL (½ dose)
Phantom
Cadaver
Statistical Reconstruction Improvements in CNR by a factor ~1.4-2.2× at ½ dose for soft tissue imaging Fair comparison achieved by matching resolution w.r.t. low-contrast target
Dose Reduction Strategy Lower tube current, then go sparse Sparse advantage in overcoming electronic noise Crossover point function of imaging task, and electronic vs quantum noise levels
Advanced Modeling Scatter correction Polyenergetic spectrum Electronic noise model
Conclusion & Future Work
20 40 60 80 100 1200
2
4
6
8
10
12
14
16
mAs
CN
R
100% P
50% P
120 mAs 15 mAs
100% P
50% P