Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka,...
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Transcript of Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka,...
![Page 1: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/1.jpg)
Ultrasonic Attenuation TomographyBased on Log-Spectrum Analysis
Radovan Jiřík, Rainer Stotzka, Torfinn Taxt
Brno University of TechnologyDepartment of Biomedical EngineeringBrno, CZECH REPUBLIC
University of BergenDepartment of BiomedicineBergen, NORWAY
Forschungszentrum KarlsruheInstitute for Data-Processing and ElectronicsEggenstein, GERMANY
![Page 2: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/2.jpg)
1. Introduction
Aim:
ultrasonic attenuation tomographyfor breast cancer diagnosis using
![Page 3: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/3.jpg)
1. Introduction
B-mode ultrasonic imaging• low spatial resolution• low contrast
Ultrasound computed tomography• more data available• more complicated acquisition and signal processing
Ultrasound attenuation imaging• att. coef. closely related to tissue type and pathology• tomography setup possible for mammography• correction of reflection tomography images• standalone imaging modality
![Page 4: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/4.jpg)
1. Introduction
Main idea: processing of reflected / scattered signal
sendingtransducer
l
receivingtransducer
s(t)
{tl = l / c
t
Initial study presented
{
undirected beam
![Page 5: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/5.jpg)
2. Model of RF signal
Directly transmitted signalsendingtransducer
l
receivingtransducer
s(t)
t
{tl = l / c
FFT
S(,l)
nattenuatio
lil
pulse
eeGlS ),(2)(),(
mean attenuation coefficient
![Page 6: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/6.jpg)
s(t)
t
2. Model of RF signal
Reflected / scattered signalsendingtransducer
receivingtransducer
{FFT
S(,l1+l2)
nattenuatio
llill
pulse
eeGllS ),(2)(
2121
21
)(),(
l1
l2
![Page 7: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/7.jpg)
3. Method
Segment of reflected / scattered signal - amplitude spectrum:
2)(
21
21
)(),(ll
eGllS
Log-spectrum:
2
)()(log),(log 2121 llGllS
Modified log-spectrum:
2
)(),(log 2121 llllSM
Linear regression => (mean attenuation coefficient along the path l1+l2)
0
0
![Page 8: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/8.jpg)
3. Method
x
y{
1
{
n
{
2
{
3
In the end – mean of thecumulated values calculated
For each pixel - all combinations of sending and receiving positions
![Page 9: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/9.jpg)
3. Method
Method analysis
• All segments with the contribution of the computed pixel cumulated
• Contribution of other pixels does not average out• Values shifted closer to the mean attenuation
coefficient in the image• Influence of neighboring pixels
• Estimation of : for non-sparse reflectors / scatterers log-spectrum not a linear function, but still a monotonous function
i
![Page 10: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/10.jpg)
4. Results
Standard unfiltered backprojection
New attenuation imaging technique
![Page 11: Ultrasonic Attenuation Tomography Based on Log-Spectrum Analysis Radovan Jiřík, Rainer Stotzka, Torfinn Taxt Brno University of Technology Department of.](https://reader036.fdocuments.in/reader036/viewer/2022082518/56649eec5503460f94bfd7b0/html5/thumbnails/11.jpg)
5. Conclusion
• Not only directly transmitted signal processed, reflected / scattered signal used in addition => significantly more data
• Attenuation images with less geometry distortion than the backprojection algorithm
• Simplifying assumptions used
Further research• huge set of linear / nonlinear equations• “Filtered backprojection” algorithm for non-straight
propagation lines ???• More complete model (non-sparse reflectors / scatterers)