Implementing the probe beam deflection technique for acoustic sensing in photoacoustic and ultrasound imaging Ronald A. Barnes Jr. The University of Texas.

Slides:



Advertisements
Similar presentations
Introduction Acoustic radiation forces on particles within standing waves are used in processes such as particle separation, fractionation and agglomeration.
Advertisements

I2 Medical imaging.
The Asymptotic Ray Theory
Six-week project Lauren Villemaire MBP 3970Z Department of Medical Biophysics University of Western Ontario.
Foundations of Medical Ultrasonic Imaging
Hyperspectral two-photon near- infrared cancer imaging at depth Nikolay S. Makarov, Jean Starkey, Mikhail Drobizhev, Aleksander Rebane, Montana State University,
Opto-Acoustic Imaging Peter E. Andersen Optics and Fluid Dynamics Department Risø National Laboratory Roskilde, Denmark
1 Two methods for modelling the propagation of terahertz radiation in a layered structure. GILLIAN C. WALKER 1*, ELIZABETH BERRY 1, STEPHEN W. SMYE 2,
Laser Anemometry P M V Subbarao Professor Mechanical Engineering Department Creation of A Picture of Complex Turbulent Flows…..
PHOTOACOUSTIC PROBE FOR TUMOR DETECTION
Two dimensional elasticity mapping of partially cross-linked rabbit corneas using optical coherence elastography Jiasong Li 1, Manmohan Singh 1, Srilatha.
Frequency Domain Optical Coherence Tomography (FDOCT) Joon S Kim IMSURE Summer Research Fellow At Beckman Laser Institute University of California at Irvine.
ECE 501 Introduction to BME
Apertureless Scanning Near-field Optical Microscopy: a comparison between homodyne and heterodyne approaches Journal Club Presentation – March 26 th, 2007.
In Vivo Evaluation of a Mechanically-Oscillating Dual- Mode Applicator for Ultrasound Imaging and Thermal Ablation Neil Owen et al. IEEE Transactions on.
Photo Acoustic Effect And its usage for spectroscopy.
Development of a thermal cooling system for a PMT (Photo Multiplier Tube) Summer Researcher Yasmine Salas Colorado State University Advisor: Dr. Julia.
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
Common types of spectroscopy
1 Opto-Acoustic Imaging 台大電機系李百祺. 2 Conventional Ultrasonic Imaging Spatial resolution is mainly determined by frequency. Fabrication of high frequency.
3/13/2009IB Physics HL 21 Ultrasound Medical Imaging Physics – IB Objectives I.2.7Describe the principles of the generation and the detection of ultrasound.
Photo-Thermal Coherent Confocal Microscope This work is supported in part by the Center for Subsurface Sensing and Imaging Systems, under the Engineering.
10/17/97Optical Diffraction Tomography1 A.J. Devaney Department of Electrical Engineering Northeastern University Boston, MA USA
Building Three-Dimensional Images Using a Time-Reversal Chaotic Cavity
BMI I FS05 – Class 9 “Ultrasound Imaging” Slide 1 Biomedical Imaging I Class 9 – Ultrasound Imaging Doppler Ultrasonography; Image Reconstruction 11/09/05.
Abstract: A laser based ultrasonic technique for the inspection of thin plates and membranes is presented, in which Lamb waves are excited using a pulsed.
Multi Frequency Laser Driver for Near Infrared Optical Spectroscopy in Biomedical Application Chenpeng Mu Department of Electrical and Computer Engineering,
Example problem 1 Example problem 2
Turbidity Suppression in a Scattering Medium via Digital Optical Phase Conjugation Mehdi Azimipour, Farid Atry, Ramin Pashaie Department of Electrical.
Introduction to the Physics Echocardiography Introduction to the Physics Echocardiography Jose L. Rivera, M.D. January 9, 2010.
BioE153:Imaging As An Inverse Problem Grant T. Gullberg
Sowmya Vasa, Umar Alqasemi, Aditya Bhargava. Objectives This paper aims in bringing out a novel light microscopy method called Focal Modulation Microscopy.
Ultrasound Simulations using REC and SAFT Presenter: Tony Podkowa November 13, 2012 Advisor: Dr José R. Sánchez Department of Electrical and Computer Engineering.
Fast Electron Temperature Scaling and Conversion Efficiency Measurements using a Bremsstrahlung Spectrometer Brad Westover US-Japan Workshop San Diego,
Electromagnetic Waves
Atomic Fluorescence Spectroscopy. Background l First significant research by Wineforder and Vickers in 1964 as an analytical technique l Used for element.
Numerical Simulations of Laser-Tissue Interactions Shannon M. Mandel Sophomore Intense Laser Physics Theory Unit Illinois State University Supervisor.
University of Kurdistan Food Quality Evaluation Methods (FQEM) Lecturer: Kaveh Mollazade, Ph.D. Department of Biosystems Engineering, Faculty of Agriculture,
Pegasus Lectures, Inc. COPYRIGHT 2006 Volume I Companion Presentation Frank R. Miele Pegasus Lectures, Inc. Ultrasound Physics & Instrumentation 4 th Edition.
Ch 10 Pages ; Lecture 24 – Introduction to Spectroscopy.
Ultrasound Basis Michel Slama Amiens.
1 Resolution Enhancement Compression- Synthetic Aperture Focusing Techniques Student: Hans Bethe Advisor: Dr. Jose R. Sanchez Bradley University Department.
A STUDENT’S EXPERIMENT WITH MULTIPLE REFLECTIONS AND REFRACTIONS ON A GLASS PLATE AND VALIDATION OF THE FRESNEL’S EQUATIONS N. Mahmudi 1, S. Rendevski.
Photoacoustic Tomography The Future Of Medical Imaging Techniques
TISSUE HARMONIC IMAGING (THI)
2/17/11 Robert Kim, BME, AMS Steven Su, BME, AMS Saurabh Vyas, BME, EE Interventional Photoacoustic Registration.
Date of download: 5/31/2016 Copyright © 2016 SPIE. All rights reserved. Schematic diagram of tissue-mimicking phantom and rabbit aorta specimen for imaging.
Date of download: 5/31/2016 Copyright © 2016 SPIE. All rights reserved. Example of a time-variant filter F(t,ω) designed using Eq. (9) to compensate for.
Date of download: 6/2/2016 Copyright © 2016 SPIE. All rights reserved. Drawing of the distal face of the fiber ferrule. The OIR source fiber is located.
N. Kuo, H.J. Kang, T. DeJournett, J. Spicer, and E. Boctor Proc. SPIE 7964, (2011); doi: / Photoacoustic Imaging of Prostate Brachytherapy.
4/7/11 Robert Kim, BME, AMS Steven Su, BME, AMS Saurabh Vyas, BME, EE Mentors: Dr. Emad Boctor, Dr Russell Taylor Special Thanks to: Nathanael Kuo Interventional.
10fs laser pulse propagation in air Conclusion The properties of femtosecond laser pulse propagation over a long distance (up to 100m) were studied for.
Date of download: 7/2/2016 Copyright © 2016 SPIE. All rights reserved. Simulation of the ablation cross section by a sequence of laser pulses with an ideal.
NUR INANI BINTI MOHD RUZLAN A Tissue harmonic imaging is a technique in ultrasonography that provides images of better quality as compared to conventional.
Center for Biomedical Optics and New Laser Systems Modeling OCT using the extended Huygens-Fresnel principle Peter E. Andersen Optics and Fluid Dynamics.
1 Opto-Acoustic Imaging 台大電機系李百祺. 2 Conventional Ultrasonic Imaging Spatial resolution is mainly determined by frequency. Fabrication of high frequency.
Date of download: 7/9/2016 Copyright © 2016 SPIE. All rights reserved. Schematic of the experimental setup: APD, avalanche photodiode; BS, beamsplitter;
Date of download: 7/9/2016 Copyright © 2016 SPIE. All rights reserved. Experimental configuration of the PAT setup coregistered with the DOT system. The.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. The implementation of the angular spectrum of plane waves method in the finite.
Date of download: 9/17/2016 Copyright © 2016 SPIE. All rights reserved. Experimental layout. (a) Schematic of phantom showing the cross-sectional and overhead.
Imaging of propagating wave fronts resulting from ultrasonic pulses incident on heel bones using refracto-vibrometry Acoustical Society of America Meeting.
Numerical Simulations of Laser-Tissue Interactions
Optical Coherence Tomography
Tianshuai Liu1, Junyan Rong1, Peng Gao1, Hongbing Lu1
Photo acoustic tomography
Point Detector Aperture
Volume I Companion Presentation Frank R. Miele Pegasus Lectures, Inc.
Mont-Carlo simulation of OCT structural images of subcutaneous
Theoretical Background Challenges and Significance
Presentation transcript:

Implementing the probe beam deflection technique for acoustic sensing in photoacoustic and ultrasound imaging Ronald A. Barnes Jr. The University of Texas at San Antonio This work is a collaboration between The University of Texas at San Antonio and The University of Texas Health Science Center.

Outline Introduction Background Modeling (MATLAB) –Acoustic Wave Propagation –Ray Tracing Simulation (MATLAB) –Optimum Sensor Topology –Optimum Beam Topology –Quadrant Photodiode Simulation –Acoustic Wave Directionality Measurement –Sensor Frequency Response Visualization (ParaView and MATLAB) Conclusion

Introduction What is Photoacoustic Tomography? Photoacoustic Tomography (PAT) is accomplished by measuring the propagating acoustic energy radiated from a sample of tissue whose thermal expansion is invoked by a pulse laser. An image of the tissue composition is reconstructed based on the measurement of the of this acoustic energy. What is the Probe Beam Deflection Technique? The Probe Beam Deflection Technique (PBDT) is sensing topology that uses probe beam lasers and there deflection and refraction to measure the properties of the propagating acoustic wave, through the implementation of a Quadrant Photodiode (QPD). Why is Modeling and Simulation important for this project? To develop an efficient algorithm for reconstruction of a tissue composition image, one must understand the interaction between probe beam and propagating acoustic wave front. A ray tracing simulation in combination with an acoustic wave simulation will allow for the prediction of beam deflection or refraction for various experimental topologies and implementations.

Background (PAT) Light enters a scattering medium (Ex. Tissue Phantom) where a portion of the energy is absorbed by the tissue in the form of heat, this produces thermal expansion. If the temperature increase inside the phantom occurs at a faster rate then the thermal relaxation time of the tissue, an acoustic wave will propagate as a result of the photo-acoustic effect. This acoustic wave produced is a wideband ultrasonic transmission and to date is measured with piezoelectric transducers.

PAT Applications Melanoma detection Photoacoustic tomography of gene expression. Doppler photoacoustic tomography for flow measurement. Photoacoustic and thermoacoustic tomography of the brain Low-background thermoacoustic molecular imaging. [2]. Prospects of photoacoustic tomography, Lihong V. Wang

Photoacoustic vs. Other Contrast Methods Contrast Method Bandwidth (Hz)Primary Contrast Penetration Depth (mm) Axial Resolution (um) Lateral Resolution (um) Photoacoustic microscopy50 MOptical absorption31545 Photoacoustic microscopy5 MOptical absorption50700 Confocal microscopyFluorescence, scattering Two-photon microscopyFluorescence Optical coherence tomography50 TOptical scattering Scanning Laser Acoustic Microscopy300 MUltrasonic scattering220 Acoustic microscopy50 MUltrasonic scattering Ultrasonography5 MUltrasonic scattering60300 [1] Optical Imaging Laboratory, Department of Biomedical Engineering, Washington University in St. Louis.

Background (PBDT) PBDT is implemented by focusing probe beams through an enclosure filled with a propagation medium. As an acoustic wave travels through the medium the refractive index is changed relative to the pressure gradient produced by the wave. The probe beam deflects and refracts as it interacts with the refractive index profile along its beam path. The probe beam deflection technique offers various advantages when compared to transducers, these include: Wave front directionality measurement, passive sensing, and low implementation cost.

Development of a Model Step 1: Produce a model of acoustic wave propagation in homogeneous and heterogeneous mediums based on the 2 nd order PDE governing acoustic wave propagation. Step 2: Modify this model in such a way that all parameters are adjustable. This includes: Initial acoustic wave magnitude, propagation medium properties, acoustic wave frequency, etc. Step 3: Convert the pressure values in the four dimensional dataset (3 dim. for space and 1 for time) to refractive index using the lorentz-lorenz relation. Step 4: Develop a ray tracing simulation to trace a bundle of rays through the previously created dataset using the vector form of Snells law. This simulation should have adjustable parameters which include: initial ray origin (for all rays that make up beam), initial ray intensity, and initial ray direction.

Model Setup

MATLAB Visualization

Method for Ray Trace Simulation (PBDT) The nature of Snells law allows the PBDT method to determine the propagation direction of the wavefront in relation to the probe beam. This is a distinct advantage over piezoelectrics whose measurement ability is limited to distance from transducer to acoustic wave source.

Visual Example of Ray Trace

Probe Beam Orientations

Quadrant Photodiode Concept

Beam Intersection on QPD Surface (Simulation)

MATLAB Visualization

QPD X SIGNAL QPD Y SIGNAL

Experimental Implementation

Probe Beam Orientations (Experiment)

Experimental Results A B C

Future Work Define optimum beam and sensor topologies for experimental implementation of PBDT derived from simulation. Define the frequency response of PBDT and compare to the frequency response to commercially available transducers. Develop reconstruction algorithm based on integrating line detectors as proposed by G. Paltauf but with added angular information.

Acknowledgments NSF grant (HRD ), Drs. Demetris Kazakos and Richard Smith, project managers. PREM Grant # DMR

References André Conjusteau, Saher Maswadi, Sergey Ermilov, Hans-Peter Brecht, Norman Barsalou, Randolph D. Glickman and Alexander A. Oraevsky, "Detection of gold-nanorod targeted pathogens using optical and piezoelectric optoacoustic sensors: comparative study", Proc. SPIE 7177, 71771P (2009); doi: / B. E. Treeby and B. T. Cox, "A k-space Green's function solution for acoustic initial value problems in homogeneous media with power law absorption," J. Acoust. Soc. Am., vol. 129, no. 6, pp , B. E. Treeby, E. Z. Zhang, and B. T. Cox, "Photoacoustic tomography in absorbing acoustic media using time reversal," Inverse Prob., vol. 26, no. 11, p , B. E. Treeby and B. T. Cox, "Modeling power law absorption and dispersion for acoustic propagation using the fractional Laplacian," J. Acoust. Soc. Am., vol. 127, no. 5, pp , 2010 B. E. Treeby and B. T. Cox, "k-Wave: MATLAB toolbox for the simulation and reconstruction of photoacoustic wave-fields," J. Biomed. Opt., vol. 15, no. 2, p , B. T. Cox and B. E. Treeby, "Artifact trapping during time reversal photoacoustic imaging for acoustically heterogeneous media," IEEE Trans. Med. Imaging, vol. 29, no. 2, pp , B. T. Cox, S. Kara, S. R. Arridge, and P. C. Beard, "k-space propagation models for acoustically heterogeneous media: Application to biomedical photoacoustics," J. Acoust. Soc. Am., vol. 121, no. 6, pp , 2007 B. T. Cox and P. C. Beard, "Fast calculation of pulsed photoacoustic fields in fluids using k-space methods," J. Acoust. Soc. Am., vol. 177, no. 6, pp , Wang, L. V., Ed.. Photoacoustic Imaging and Spectroscopy. Taylor & Francis, 2009.

Questions??