MB-JASS D Reconstruction. Hannes Hofmann March 2006

Size: px
Start display at page:

Download "MB-JASS D Reconstruction. Hannes Hofmann March 2006"

Transcription

1 MB-JASS D Reconstruction Hannes Hofmann March 2006

2 Outline Projections Radon Transform Fourier-Slice-Theorem Filtered Backprojection Ramp Filter Mar 2006 Hannes Hofmann 2

3 Parallel Projections X-Rays are attenuated as they propagate through the human body Mar 2006 Hannes Hofmann 3

4 Radon Transform The signal p t is the Radon transform of the object p t = f x, y xcos ysin t dx dy Set of line integrals along the direction at the distance t from the origin Mar 2006 Hannes Hofmann 4

5 Radon Transform (2) A simple image (left) and the sinogram (right) produced by applying the Radon transform (180 projections with an angle of 1 degree) Mar 2006 Hannes Hofmann 5

6 Unfiltered BP Ok, that's bad. But we used only 18 projections Mar 2006 Hannes Hofmann 6

7 Unfiltered BP (2) Now we used all 180 projections. Still poor image quality Mar 2006 Hannes Hofmann 7

8 Fourier Slice Theorem t p t f x, y F u,v P w Projection under angle Slice under in freq. domain Mar 2006 Hannes Hofmann 8

9 Fourier Slice Theorem (2) Projection of f x, y in y direction is p =0 x = f x, y dy p =0 x

10 Fourier Slice Theorem (2) Projection of f x, y : p =0 x = The Fourier transform of f x, y is F u, v = f x, y e 2 i xu yv dx dy f x, y dy

11 Fourier Slice Theorem (2) Projection of f x, y : The Fourier transform of f x, y is F u, v = The slice s u is then s u =F u,0 = [ = = p =0 x = f x, y e 2 i xu yv dx dy which is just the Fourier transform of Formal derivation see e.g. Kak & Slaney f x, y e i2 xu dx dy f x, y dy]e i2 xu dx p =0 t e i2 tu dt f x, y dy p =0 x

12 Fourier Slice Theorem (3) t p t f x, y F u,v P w Projection under many angles Slices in frequency domain Mar 2006 Hannes Hofmann 12

13 FST - Regridding Projection data lies on circles (dots) and has to be interpolated to a Cartesian coordinate system Interpolation gets worse with increasing u & v v Errors in high-frequency regions, i.e. regions with high detail u Frequency domain Mar 2006 Hannes Hofmann 13

14 Unfiltered Backprojection Mar 2006 Hannes Hofmann 14

15 Solution: Filtering Ideal situation Fourier Slice Theorem Mar 2006 Hannes Hofmann 15

16 Solution: Filtering Ideal situation Fourier Slice Theorem The ideal is approximated by a weighting (highpass)

17 Filtered Backprojection Switch to polar coordinates 2 f x, y = 0 0 F w, e i2 xcos ysin w dw d = i2 xcos 0 0 F w, e ysin w dw d i2 0 0 F w, e xcos ysin w dw d

18 Filtered Backprojection Switch to polar coordinates 2 f x, y = 0 0 F w, e i2 xcos ysin w dw d = i2 xcos 0 0 F w, e ysin w dw d i2 0 0 F w, e xcos ysin w dw d 180 symmetry F u, =F u, f x, y = 0 [ F w, e i2 wt w dw]d t=xcos ysin Mar 2006 Hannes Hofmann 18

19 Filtered Backprojection (2) Apply Fourier Slice Theorem f x, y = 0 [ P w e i2 wt w dw]d Which can be written as f x, y = 0 Q t d Q t = P w e i2 wt w dw Q is the filtered projection with filter function w (in frequency domain) Mar 2006 Hannes Hofmann 19

20 Ramp Filter Convolution in frequency domain High-pass, emphasizes noise Mar 2006 Hannes Hofmann 20

21 Filter Results Attenuation profile of a cylinder p t Filtered attenuation profile p t K t convolution Mar 2006 Hannes Hofmann 21

22 Filtered BP: Result Reconstruction using ramp filtered backprojection (180 projections) Mar 2006 Hannes Hofmann 22

23 Sharp Kernel Bone image: use sharp kernel high resolution high noise Mar 2006 Hannes Hofmann 23

24 Soft Kernel Soft tissue: use soft kernel lower resolution less noise Mar 2006 Hannes Hofmann 24

25 Filtered Backprojection Mar 2006 Hannes Hofmann 25

26 Thanks Thank you for your attention. Do you have any questions? Mar 2006 Hannes Hofmann 26

27 References A. C. Kak and Malcolm Slaney, Principles of Computerized Tomographic Imaging. Society of Industrial and Applied Mathematics, 2001 S. Horbelt, M. Liebling, M. Unser: Filter design for filtered back-projection guided by the interpolation model, Proceedings of the SPIE International Symposium on Medical Imaging: Image Processing (MI'02), San Diego CA, USA, February 24-28, 2002, vol. 4684, Part II, pp J. Hornegger, D. Paulus: Slides to Medical Image Processing B. Heismann: Slides to Medical Imaging Slice_Reconstruction.html kprojection.htm Mar 2006 Hannes Hofmann 27

Image Reconstruction from Projection

Image Reconstruction from Projection Image Reconstruction from Projection Reconstruct an image from a series of projections X-ray computed tomography (CT) Computed tomography is a medical imaging method employing tomography where digital

More information

EE 4372 Tomography. Carlos E. Davila, Dept. of Electrical Engineering Southern Methodist University

EE 4372 Tomography. Carlos E. Davila, Dept. of Electrical Engineering Southern Methodist University EE 4372 Tomography Carlos E. Davila, Dept. of Electrical Engineering Southern Methodist University EE 4372, SMU Department of Electrical Engineering 86 Tomography: Background 1-D Fourier Transform: F(

More information

Lecture 9 February 2, 2016

Lecture 9 February 2, 2016 MATH 262/CME 372: Applied Fourier Analysis and Winter 26 Elements of Modern Signal Processing Lecture 9 February 2, 26 Prof. Emmanuel Candes Scribe: Carlos A. Sing-Long, Edited by E. Bates Outline Agenda:

More information

The Theory of Diffraction Tomography

The Theory of Diffraction Tomography The Theory of Diffraction Tomography Paul Müller 1, Mirjam Schürmann, and Jochen Guck Biotechnology Center, Technische Universität Dresden, Dresden, Germany (Dated: October 10, 2016) Abstract arxiv:1507.00466v3

More information

Topics. Example. Modulation. [ ] = G(k x. ] = 1 2 G ( k % k x 0) G ( k + k x 0) ] = 1 2 j G ( k x

Topics. Example. Modulation. [ ] = G(k x. ] = 1 2 G ( k % k x 0) G ( k + k x 0) ] = 1 2 j G ( k x Topics Bioengineering 280A Principles of Biomedical Imaging Fall Quarter 2008 CT/Fourier Lecture 3 Modulation Modulation Transfer Function Convolution/Multiplication Revisit Projection-Slice Theorem Filtered

More information

1 Radon Transform and X-Ray CT

1 Radon Transform and X-Ray CT Radon Transform and X-Ray CT In this section we look at an important class of imaging problems, the inverse Radon transform. We have seen that X-ray CT (Computerized Tomography) involves the reconstruction

More information

Topics. Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2006 CT/Fourier Lecture 2

Topics. Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2006 CT/Fourier Lecture 2 Bioengineering 280A Principles of Biomedical Imaging Fall Quarter 2006 CT/Fourier Lecture 2 Topics Modulation Modulation Transfer Function Convolution/Multiplication Revisit Projection-Slice Theorem Filtered

More information

Part 2 Introduction to Microlocal Analysis

Part 2 Introduction to Microlocal Analysis Part 2 Introduction to Microlocal Analysis Birsen Yazıcı& Venky Krishnan Rensselaer Polytechnic Institute Electrical, Computer and Systems Engineering March 15 th, 2010 Outline PART II Pseudodifferential(ψDOs)

More information

Hamburger Beiträge zur Angewandten Mathematik

Hamburger Beiträge zur Angewandten Mathematik Hamburger Beiträge zur Angewandten Mathematik Error Estimates for Filtered Back Projection Matthias Beckmann and Armin Iske Nr. 2015-03 January 2015 Error Estimates for Filtered Back Projection Matthias

More information

Part 2 Introduction to Microlocal Analysis

Part 2 Introduction to Microlocal Analysis Part 2 Introduction to Microlocal Analysis Birsen Yazıcı & Venky Krishnan Rensselaer Polytechnic Institute Electrical, Computer and Systems Engineering August 2 nd, 2010 Outline PART II Pseudodifferential

More information

Topics. EM spectrum. X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection

Topics. EM spectrum. X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection Bioengineering 28A Principles of Biomedical Imaging Fall Quarter 25 X-Rays/CT Lecture Topics X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection

More information

Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2005 X-Rays/CT Lecture 1. Topics

Bioengineering 280A Principles of Biomedical Imaging. Fall Quarter 2005 X-Rays/CT Lecture 1. Topics Bioengineering 28A Principles of Biomedical Imaging Fall Quarter 25 X-Rays/CT Lecture Topics X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection

More information

A pointwise limit theorem for filtered backprojection in computed tomography

A pointwise limit theorem for filtered backprojection in computed tomography A pointwise it theorem for filtered backprojection in computed tomography Yangbo Ye a) Department of Mathematics University of Iowa Iowa City Iowa 52242 Jiehua Zhu b) Department of Mathematics University

More information

Maximal Entropy for Reconstruction of Back Projection Images

Maximal Entropy for Reconstruction of Back Projection Images Maximal Entropy for Reconstruction of Back Projection Images Tryphon Georgiou Department of Electrical and Computer Engineering University of Minnesota Minneapolis, MN 5545 Peter J Olver Department of

More information

Medical Imaging. Transmission Measurement

Medical Imaging. Transmission Measurement Medical Imaging Image Recontruction from Projection Prof Ed X. Wu Tranmiion Meaurement ( meaurable unknown attenuation, aborption cro-ection hadowgram ) I(ϕ,ξ) µ(x,) I = I o exp A(x, )dl L X-ra ource X-Ra

More information

LECTURES ON MICROLOCAL CHARACTERIZATIONS IN LIMITED-ANGLE

LECTURES ON MICROLOCAL CHARACTERIZATIONS IN LIMITED-ANGLE LECTURES ON MICROLOCAL CHARACTERIZATIONS IN LIMITED-ANGLE TOMOGRAPHY Jürgen Frikel 4 LECTURES 1 Today: Introduction to the mathematics of computerized tomography 2 Mathematics of computerized tomography

More information

ROI Reconstruction in CT

ROI Reconstruction in CT Reconstruction in CT From Tomo reconstruction in the 21st centery, IEEE Sig. Proc. Magazine (R.Clackdoyle M.Defrise) L. Desbat TIMC-IMAG September 10, 2013 L. Desbat Reconstruction in CT Outline 1 CT Radiology

More information

Filtering and Edge Detection

Filtering and Edge Detection Filtering and Edge Detection Local Neighborhoods Hard to tell anything from a single pixel Example: you see a reddish pixel. Is this the object s color? Illumination? Noise? The next step in order of complexity

More information

Filtering in Frequency Domain

Filtering in Frequency Domain Dr. Praveen Sankaran Department of ECE NIT Calicut February 4, 2013 Outline 1 2D DFT - Review 2 2D Sampling 2D DFT - Review 2D Impulse Train s [t, z] = m= n= δ [t m T, z n Z] (1) f (t, z) s [t, z] sampled

More information

High Performance Computing for Neutron Tomography Reconstruction

High Performance Computing for Neutron Tomography Reconstruction High Performance Computing for Neutron Tomography Reconstruction A Parallel Approach to Filtered Backprojection (FBP) Zongpu Li 1 Cain Gantt 2 1 Department of Physics and Materials Science City University

More information

Convolution Theorem Modulation Transfer Function y(t)=g(t)*h(t)

Convolution Theorem Modulation Transfer Function y(t)=g(t)*h(t) MTF = Fourier Transform of PSF Bioengineering 28A Principles of Biomedical Imaging Fall Quarter 214 CT/Fourier Lecture 4 Bushberg et al 21 Convolution Theorem Modulation Transfer Function y(t=g(t*h(t g(t

More information

Interpolation procedure in filtered backprojection algorithm for the limited-angle tomography

Interpolation procedure in filtered backprojection algorithm for the limited-angle tomography Interpolation procedure in filtered backprojection algorithm for the limited-angle tomography Aleksander Denisiuk 1 Abstract A new data completion procedure for the limited-angle tomography is proposed.

More information

The Radon Transform and the Mathematics of Medical Imaging

The Radon Transform and the Mathematics of Medical Imaging Colby College Digital Commons @ Colby Honors Theses Student Research 2012 The Radon Transform and the Mathematics of Medical Imaging Jen Beatty Colby College Follow this and additional works at: http://digitalcommons.colby.edu/honorstheses

More information

Saturation Rates for Filtered Back Projection

Saturation Rates for Filtered Back Projection Saturation Rates for Filtered Back Projection Matthias Beckmann, Armin Iske Fachbereich Mathematik, Universität Hamburg 3rd IM-Workshop on Applied Approximation, Signals and Images Bernried, 21st February

More information

Winter College on Optics: Trends in Laser Development and Multidisciplinary Applications to Science and Industry February 2013

Winter College on Optics: Trends in Laser Development and Multidisciplinary Applications to Science and Industry February 2013 2443-27 Winter College on Optics: Trends in Laser Development and Multidisciplinary Applications to Science and Industry 4-15 February 2013 Data capture and tomographic reconstruction of phase microobjects

More information

A Brief Introduction to Medical Imaging. Outline

A Brief Introduction to Medical Imaging. Outline A Brief Introduction to Medical Imaging Outline General Goals Linear Imaging Systems An Example, The Pin Hole Camera Radiations and Their Interactions with Matter Coherent vs. Incoherent Imaging Length

More information

NIH Public Access Author Manuscript Proc Soc Photo Opt Instrum Eng. Author manuscript; available in PMC 2013 December 17.

NIH Public Access Author Manuscript Proc Soc Photo Opt Instrum Eng. Author manuscript; available in PMC 2013 December 17. NIH Public Access Author Manuscript Published in final edited form as: Proc Soc Photo Opt Instrum Eng. 2008 March 18; 6913:. doi:10.1117/12.769604. Tomographic Reconstruction of Band-limited Hermite Expansions

More information

Tuesday, September 29, Page 453. Problem 5

Tuesday, September 29, Page 453. Problem 5 Tuesday, September 9, 15 Page 5 Problem 5 Problem. Set up and evaluate the integral that gives the volume of the solid formed by revolving the region bounded by y = x, y = x 5 about the x-axis. Solution.

More information

Topics. EM spectrum. X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection

Topics. EM spectrum. X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection Bioengineering 28A Principles of Biomedical Imaging Fall Quarter 24 X-Rays/CT Lecture Topics X-Rays Computed Tomography Direct Inverse and Iterative Inverse Backprojection Projection Theorem Filtered Backprojection

More information

Convolution/Modulation Theorem. 2D Convolution/Multiplication. Application of Convolution Thm. Bioengineering 280A Principles of Biomedical Imaging

Convolution/Modulation Theorem. 2D Convolution/Multiplication. Application of Convolution Thm. Bioengineering 280A Principles of Biomedical Imaging Bioengineering 8A Principles of Biomedical Imaging Fall Quarter 15 CT/Fourier Lecture 4 Convolution/Modulation Theorem [ ] e j πx F{ g(x h(x } = g(u h(x udu = g(u h(x u e j πx = g(uh( e j πu du = H( dxdu

More information

Midterm Review. Yao Wang Polytechnic University, Brooklyn, NY 11201

Midterm Review. Yao Wang Polytechnic University, Brooklyn, NY 11201 Midterm Review Yao Wang Polytechnic University, Brooklyn, NY 11201 Based on J. L. Prince and J. M. Links, Medical maging Signals and Systems, and lecture notes by Prince. Figures are from the textbook.

More information

SPATIAL RESOLUTION PROPERTIES OF PENALIZED WEIGHTED LEAST-SQUARES TOMOGRAPHIC IMAGE RECONSTRUCTION WITH MODEL MISMATCH

SPATIAL RESOLUTION PROPERTIES OF PENALIZED WEIGHTED LEAST-SQUARES TOMOGRAPHIC IMAGE RECONSTRUCTION WITH MODEL MISMATCH SPATIAL RESOLUTION PROPERTIES OF PENALIZED WEIGHTED LEAST-SQUARES TOMOGRAPHIC IMAGE RECONSTRUCTION WITH MODEL MISMATCH Jeffrey A. Fessler COMMUNICATIONS & SIGNAL PROCESSING LABORATORY Department of Electrical

More information

Microlocal Methods in X-ray Tomography

Microlocal Methods in X-ray Tomography Microlocal Methods in X-ray Tomography Plamen Stefanov Purdue University Lecture I: Euclidean X-ray tomography Mini Course, Fields Institute, 2012 Plamen Stefanov (Purdue University ) Microlocal Methods

More information

Tomography and Reconstruction

Tomography and Reconstruction Tomography and Reconstruction Lecture Overview Applications Background/history of tomography Radon Transform Fourier Slice Theorem Filtered Back Projection Algebraic techniques Measurement of Projection

More information

Edge Detection PSY 5018H: Math Models Hum Behavior, Prof. Paul Schrater, Spring 2005

Edge Detection PSY 5018H: Math Models Hum Behavior, Prof. Paul Schrater, Spring 2005 Edge Detection PSY 5018H: Math Models Hum Behavior, Prof. Paul Schrater, Spring 2005 Gradients and edges Points of sharp change in an image are interesting: change in reflectance change in object change

More information

The mathematics behind Computertomography

The mathematics behind Computertomography Radon transforms The mathematics behind Computertomography PD Dr. Swanhild Bernstein, Institute of Applied Analysis, Freiberg University of Mining and Technology, International Summer academic course 2008,

More information

Fourier Reconstruction. Polar Version of Inverse FT. Filtered Backprojection [ ] Bioengineering 280A Principles of Biomedical Imaging

Fourier Reconstruction. Polar Version of Inverse FT. Filtered Backprojection [ ] Bioengineering 280A Principles of Biomedical Imaging Fourier Reconstruction Bioengineering 280A Principles of Biomedical Imaging Fall Quarter 2014 CT/Fourier Lecture 5 F Interpolate onto Cartesian grid with appropriate density correction then take inverse

More information

The relationship between image noise and spatial resolution of CT scanners

The relationship between image noise and spatial resolution of CT scanners The relationship between image noise and spatial resolution of CT scanners Sue Edyvean, Nicholas Keat, Maria Lewis, Julia Barrett, Salem Sassi, David Platten ImPACT*, St George s Hospital, London *An MDA

More information

Geophysical Data Analysis: Discrete Inverse Theory

Geophysical Data Analysis: Discrete Inverse Theory Geophysical Data Analysis: Discrete Inverse Theory MATLAB Edition William Menke Lamont-Doherty Earth Observatory and Department of Earth and Environmental Sciences Columbia University. ' - Palisades, New

More information

1. Which of the following statements is true about Bremsstrahlung and Characteristic Radiation?

1. Which of the following statements is true about Bremsstrahlung and Characteristic Radiation? BioE 1330 - Review Chapters 4, 5, and 6 (X-ray and CT) 9/27/2018 Instructions: On the Answer Sheet, enter your 2-digit ID number (with a leading 0 if needed) in the boxes of the ID section. Fill in the

More information

Introduction to Computer Vision. 2D Linear Systems

Introduction to Computer Vision. 2D Linear Systems Introduction to Computer Vision D Linear Systems Review: Linear Systems We define a system as a unit that converts an input function into an output function Independent variable System operator or Transfer

More information

ECG782: Multidimensional Digital Signal Processing

ECG782: Multidimensional Digital Signal Processing Professor Brendan Morris, SEB 3216, brendan.morris@unlv.edu ECG782: Multidimensional Digital Signal Processing Filtering in the Frequency Domain http://www.ee.unlv.edu/~b1morris/ecg782/ 2 Outline Background

More information

Edge Detection. Computer Vision P. Schrater Spring 2003

Edge Detection. Computer Vision P. Schrater Spring 2003 Edge Detection Computer Vision P. Schrater Spring 2003 Simplest Model: (Canny) Edge(x) = a U(x) + n(x) U(x)? x=0 Convolve image with U and find points with high magnitude. Choose value by comparing with

More information

Computed Tomography Lab phyc30021 Laboratory and Computational Physics 3

Computed Tomography Lab phyc30021 Laboratory and Computational Physics 3 Computed Tomography Lab phyc30021 Laboratory and Computational Physics 3 By Joshua P. Ellis School of Physics Last compiled 8th August 2017 Contents 1. Introduction 1 1.1. Aim.............................................

More information

ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform

ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform Department of Electrical Engineering University of Arkansas ELEG 3124 SYSTEMS AND SIGNALS Ch. 5 Fourier Transform Dr. Jingxian Wu wuj@uark.edu OUTLINE 2 Introduction Fourier Transform Properties of Fourier

More information

Opto-digital tomographic reconstruction of the Wigner distribution function of complex fields

Opto-digital tomographic reconstruction of the Wigner distribution function of complex fields Opto-digital tomographic reconstruction of the Wigner distribution function of complex fields Walter D. Furlan, 1, * Carlos Soriano, 2 and Genaro Saavedra 1 1 Departamento de Óptica, Universitat de València,

More information

6: Positron Emission Tomography

6: Positron Emission Tomography 6: Positron Emission Tomography. What is the principle of PET imaging? Positron annihilation Electronic collimation coincidence detection. What is really measured by the PET camera? True, scatter and random

More information

MAP Reconstruction From Spatially Correlated PET Data

MAP Reconstruction From Spatially Correlated PET Data IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL 50, NO 5, OCTOBER 2003 1445 MAP Reconstruction From Spatially Correlated PET Data Adam Alessio, Student Member, IEEE, Ken Sauer, Member, IEEE, and Charles A Bouman,

More information

Continuous-Time Fourier Transform

Continuous-Time Fourier Transform Signals and Systems Continuous-Time Fourier Transform Chang-Su Kim continuous time discrete time periodic (series) CTFS DTFS aperiodic (transform) CTFT DTFT Lowpass Filtering Blurring or Smoothing Original

More information

Introduction to the Mathematics of Medical Imaging

Introduction to the Mathematics of Medical Imaging Introduction to the Mathematics of Medical Imaging Second Edition Charles L. Epstein University of Pennsylvania Philadelphia, Pennsylvania EiaJTL Society for Industrial and Applied Mathematics Philadelphia

More information

Radon Transform An Introduction

Radon Transform An Introduction Radon Transform An Introduction Yi-Hsuan Lin The Radon transform is widely applicable to tomography, the creation of an image from the scattering data associated to crosssectional scans of an object. If

More information

Ke Li and Guang-Hong Chen

Ke Li and Guang-Hong Chen Ke Li and Guang-Hong Chen Brief introduction of x-ray differential phase contrast (DPC) imaging Intrinsic noise relationship between DPC imaging and absorption imaging Task-based model observer studies

More information

Convolution Spatial Aliasing Frequency domain filtering fundamentals Applications Image smoothing Image sharpening

Convolution Spatial Aliasing Frequency domain filtering fundamentals Applications Image smoothing Image sharpening Frequency Domain Filtering Correspondence between Spatial and Frequency Filtering Fourier Transform Brief Introduction Sampling Theory 2 D Discrete Fourier Transform Convolution Spatial Aliasing Frequency

More information

Principles of Computed Tomography (CT)

Principles of Computed Tomography (CT) Page 298 Princiles of Comuted Tomograhy (CT) The theoretical foundation of CT dates back to Johann Radon, a mathematician from Vienna who derived a method in 1907 for rojecting a 2-D object along arallel

More information

Two-Material Decomposition From a Single CT Scan Using Statistical Image Reconstruction

Two-Material Decomposition From a Single CT Scan Using Statistical Image Reconstruction / 5 Two-Material Decomposition From a Single CT Scan Using Statistical Image Reconstruction Yong Long and Jeffrey A. Fessler EECS Department James M. Balter Radiation Oncology Department The University

More information

Nonlinear Flows for Displacement Correction and Applications in Tomography

Nonlinear Flows for Displacement Correction and Applications in Tomography Nonlinear Flows for Displacement Correction and Applications in Tomography Guozhi Dong 1 and Otmar Scherzer 1,2 1 Computational Science Center, University of Vienna, Oskar-Morgenstern-Platz 1, 1090 Wien,

More information

Section 5.6 Integration by Parts

Section 5.6 Integration by Parts .. 98 Section.6 Integration by Parts Integration by parts is another technique that we can use to integrate problems. Typically, we save integration by parts as a last resort when substitution will not

More information

Error Estimates and Convergence Rates for Filtered Back Projection Reconstructions

Error Estimates and Convergence Rates for Filtered Back Projection Reconstructions Universität Hamburg Dissertation Error Estimates and Convergence ates for Filtered Back Projection econstructions Dissertation zur Erlangung des Doktorgrades an der Fakultät für Mathematik, Informatik

More information

BME I5000: Biomedical Imaging

BME I5000: Biomedical Imaging BME I5000: Biomedical Imaging Lecture 9 Magnetic Resonance Imaging (imaging) Lucas C. Parra, parra@ccny.cuny.edu Blackboard: http://cityonline.ccny.cuny.edu/ 1 Schedule 1. Introduction, Spatial Resolution,

More information

AREA FUNCTION IMAGING IN TWO-DIMENSIONAL UL1RASONIC. COMPUiERIZED TOMOGRAPHY. L. S. Koo, H. R. Shafiee, D. K. Hsu, S. J. Wormley, and D. 0.

AREA FUNCTION IMAGING IN TWO-DIMENSIONAL UL1RASONIC. COMPUiERIZED TOMOGRAPHY. L. S. Koo, H. R. Shafiee, D. K. Hsu, S. J. Wormley, and D. 0. AREA FUNCTION IMAGING IN TWO-DIMENSIONAL UL1RASONIC COMPUiERIZED TOMOGRAPHY L. S. Koo, H. R. Shafiee, D. K. Hsu, S. J. Wormley, and D. 0. Thompson Ames Laboratory, US DOE Iowa State University Ames, la

More information

Reconstruction for Proton Computed Tomography: A Monte Carlo Study

Reconstruction for Proton Computed Tomography: A Monte Carlo Study Reconstruction for Proton Computed Tomography: A Monte Carlo Study T Li, Z. Liang, K. Mueller, J. Heimann, L. Johnson, H. Sadrozinski, A. Seiden, D. Williams, L. Zhang, S. Peggs, T. Satogata, V. Bashkirov,

More information

1 st ORDER O.D.E. EXAM QUESTIONS

1 st ORDER O.D.E. EXAM QUESTIONS 1 st ORDER O.D.E. EXAM QUESTIONS Question 1 (**) 4y + = 6x 5, x > 0. dx x Determine the solution of the above differential equation subject to the boundary condition is y = 1 at x = 1. Give the answer

More information

Gaussian derivatives

Gaussian derivatives Gaussian derivatives UCU Winter School 2017 James Pritts Czech Tecnical University January 16, 2017 1 Images taken from Noah Snavely s and Robert Collins s course notes Definition An image (grayscale)

More information

Chapter 4: Filtering in the Frequency Domain. Fourier Analysis R. C. Gonzalez & R. E. Woods

Chapter 4: Filtering in the Frequency Domain. Fourier Analysis R. C. Gonzalez & R. E. Woods Fourier Analysis 1992 2008 R. C. Gonzalez & R. E. Woods Properties of δ (t) and (x) δ : f t) δ ( t t ) dt = f ( ) f x) δ ( x x ) = f ( ) ( 0 t0 x= ( 0 x0 1992 2008 R. C. Gonzalez & R. E. Woods Sampling

More information

Neutron and Gamma Ray Imaging for Nuclear Materials Identification

Neutron and Gamma Ray Imaging for Nuclear Materials Identification Neutron and Gamma Ray Imaging for Nuclear Materials Identification James A. Mullens John Mihalczo Philip Bingham Oak Ridge National Laboratory Oak Ridge, Tennessee 37831-6010 865-574-5564 Abstract This

More information

ITERATIVE METHODS IN LARGE FIELD ELECTRON MICROSCOPE TOMOGRAPHY. Xiaohua Wan

ITERATIVE METHODS IN LARGE FIELD ELECTRON MICROSCOPE TOMOGRAPHY. Xiaohua Wan ITERATIVE METHODS IN LARGE FIELD ELECTRON MICROSCOPE TOMOGRAPHY Xiaohua Wan wanxiaohua@ict.ac.cn Institute of Computing Technology, Chinese Academy of Sciences Outline Background Problem Our work Future

More information

Chap. 15 Radiation Imaging

Chap. 15 Radiation Imaging Chap. 15 Radiation Imaging 15.1 INTRODUCTION Modern Medical Imaging Devices Incorporating fundamental concepts in physical science and innovations in computer technology Nobel prize (physics) : 1895 Wilhelm

More information

Statistical Tomographic Image Reconstruction Methods for Randoms-Precorrected PET Measurements

Statistical Tomographic Image Reconstruction Methods for Randoms-Precorrected PET Measurements Statistical Tomographic Image Reconstruction Methods for Randoms-Precorrected PET Measurements by Mehmet Yavuz A dissertation submitted in partial fulfillment of the requirements for the degree of Doctor

More information

Lecture 4 Filtering in the Frequency Domain. Lin ZHANG, PhD School of Software Engineering Tongji University Spring 2016

Lecture 4 Filtering in the Frequency Domain. Lin ZHANG, PhD School of Software Engineering Tongji University Spring 2016 Lecture 4 Filtering in the Frequency Domain Lin ZHANG, PhD School of Software Engineering Tongji University Spring 2016 Outline Background From Fourier series to Fourier transform Properties of the Fourier

More information

Kernel-based Image Reconstruction from scattered Radon data by (anisotropic) positive definite functions

Kernel-based Image Reconstruction from scattered Radon data by (anisotropic) positive definite functions Kernel-based Image Reconstruction from scattered Radon data by (anisotropic) positive definite functions Stefano De Marchi 1 February 5, 2016 1 Joint work with A. Iske (Hamburg, D), A. Sironi (Lousanne,

More information

Foundations of Image Science

Foundations of Image Science Foundations of Image Science Harrison H. Barrett Kyle J. Myers 2004 by John Wiley & Sons,, Hoboken, 0-471-15300-1 1 VECTORS AND OPERATORS 1 1.1 LINEAR VECTOR SPACES 2 1.1.1 Vector addition and scalar multiplication

More information

Review Smoothing Spatial Filters Sharpening Spatial Filters. Spatial Filtering. Dr. Praveen Sankaran. Department of ECE NIT Calicut.

Review Smoothing Spatial Filters Sharpening Spatial Filters. Spatial Filtering. Dr. Praveen Sankaran. Department of ECE NIT Calicut. Spatial Filtering Dr. Praveen Sankaran Department of ECE NIT Calicut January 7, 203 Outline 2 Linear Nonlinear 3 Spatial Domain Refers to the image plane itself. Direct manipulation of image pixels. Figure:

More information

COMPRESSIVE OPTICAL DEFLECTOMETRIC TOMOGRAPHY

COMPRESSIVE OPTICAL DEFLECTOMETRIC TOMOGRAPHY COMPRESSIVE OPTICAL DEFLECTOMETRIC TOMOGRAPHY Adriana González ICTEAM/UCL March 26th, 214 1 ISPGroup - ICTEAM - UCL http://sites.uclouvain.be/ispgroup Université catholique de Louvain, Louvain-la-Neuve,

More information

ON A CLASS OF GENERALIZED RADON TRANSFORMS AND ITS APPLICATION IN IMAGING SCIENCE

ON A CLASS OF GENERALIZED RADON TRANSFORMS AND ITS APPLICATION IN IMAGING SCIENCE ON A CLASS OF GENERALIZED RADON TRANSFORMS AND ITS APPLICATION IN IMAGING SCIENCE T.T. TRUONG 1 AND M.K. NGUYEN 2 1 University of Cergy-Pontoise, LPTM CNRS UMR 889, F-9532, France e-mail: truong@u-cergy.fr

More information

Convergence of Particle Filtering Method for Nonlinear Estimation of Vortex Dynamics

Convergence of Particle Filtering Method for Nonlinear Estimation of Vortex Dynamics Convergence of Particle Filtering Method for Nonlinear Estimation of Vortex Dynamics Meng Xu Department of Mathematics University of Wyoming February 20, 2010 Outline 1 Nonlinear Filtering Stochastic Vortex

More information

4.4 Magnetic Resonance Imaging. Fig. 4.34: An attenuation

4.4 Magnetic Resonance Imaging. Fig. 4.34: An attenuation Fig. 4.34: An attenuation reconstruction obtained by using the frequency-shift method. (From [Kak79J.) grams. In addition, the design of a program to automatically diagnose breast tomograms based on the

More information

Fourier Series Representation of

Fourier Series Representation of Fourier Series Representation of Periodic Signals Rui Wang, Assistant professor Dept. of Information and Communication Tongji University it Email: ruiwang@tongji.edu.cn Outline The response of LIT system

More information

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea

2017 Water Reactor Fuel Performance Meeting September 10 (Sun) ~ 14 (Thu), 2017 Ramada Plaza Jeju Jeju Island, Korea Feasibility Study of using Gamma Emission Tomography for Identification of Leaking Fuel Rods in Commercial Fuel Assemblies P. Andersson 1, S. Holcombe 2 1 Uppsala University, Department of Physics and

More information

Digital Image Processing. Chapter 4: Image Enhancement in the Frequency Domain

Digital Image Processing. Chapter 4: Image Enhancement in the Frequency Domain Digital Image Processing Chapter 4: Image Enhancement in the Frequency Domain Image Enhancement in Frequency Domain Objective: To understand the Fourier Transform and frequency domain and how to apply

More information

Regularizations of general singular integral operators

Regularizations of general singular integral operators Regularizations of general singular integral operators Texas A&M University March 19th, 2011 This talk is based on joint work with Sergei Treil. This work is accepted by Revista Matematica Iberoamericano

More information

Numerical Methods in TEM Convolution and Deconvolution

Numerical Methods in TEM Convolution and Deconvolution Numerical Methods in TEM Convolution and Deconvolution Christoph T. Koch Max Planck Institut für Metallforschung http://hrem.mpi-stuttgart.mpg.de/koch/vorlesung Applications of Convolution in TEM Smoothing

More information

ENGI Parametric Vector Functions Page 5-01

ENGI Parametric Vector Functions Page 5-01 ENGI 3425 5. Parametric Vector Functions Page 5-01 5. Parametric Vector Functions Contents: 5.1 Arc Length (Cartesian parametric and plane polar) 5.2 Surfaces of Revolution 5.3 Area under a Parametric

More information

G52IVG, School of Computer Science, University of Nottingham

G52IVG, School of Computer Science, University of Nottingham Image Transforms Fourier Transform Basic idea 1 Image Transforms Fourier transform theory Let f(x) be a continuous function of a real variable x. The Fourier transform of f(x) is F ( u) f ( x)exp[ j2πux]

More information

Feature Reconstruction in Tomography

Feature Reconstruction in Tomography Feature Reconstruction in Tomography Alfred K. Louis Institut für Angewandte Mathematik Universität des Saarlandes 66041 Saarbrücken http://www.num.uni-sb.de louis@num.uni-sb.de Wien, July 20, 2009 Images

More information

Phase Space Tomography of an Electron Beam in a Superconducting RF Linac

Phase Space Tomography of an Electron Beam in a Superconducting RF Linac Phase Space Tomography of an Electron Beam in a Superconducting RF Linac Tianyi Ge 1, and Jayakar Thangaraj 2, 1 Department of Physics and Astronomy, University of California, Los Angeles, California 90095,

More information

I Chen Lin, Assistant Professor Dept. of CS, National Chiao Tung University. Computer Vision: 4. Filtering

I Chen Lin, Assistant Professor Dept. of CS, National Chiao Tung University. Computer Vision: 4. Filtering I Chen Lin, Assistant Professor Dept. of CS, National Chiao Tung University Computer Vision: 4. Filtering Outline Impulse response and convolution. Linear filter and image pyramid. Textbook: David A. Forsyth

More information

Dynamics of Quantum Many-Body Systems from Monte Carlo simulations

Dynamics of Quantum Many-Body Systems from Monte Carlo simulations s of I.N.F.N. and Physics Department, University of Trento - ITALY INT - Seattle - October 24, 2012 Collaborators s of Alessandro Roggero (Trento) Giuseppina Orlandini (Trento) Outline s of : transform

More information

Chapter 4 Image Enhancement in the Frequency Domain

Chapter 4 Image Enhancement in the Frequency Domain Chapter 4 Image Enhancement in the Frequency Domain Yinghua He School of Computer Science and Technology Tianjin University Background Introduction to the Fourier Transform and the Frequency Domain Smoothing

More information

Potentials for Dual-energy kv/mv On-board Imaging and Therapeutic Applications

Potentials for Dual-energy kv/mv On-board Imaging and Therapeutic Applications Potentials for Dual-energy kv/mv On-board Imaging and Therapeutic Applications Fang-Fang Yin Department of Radiation Oncology Duke University Medical Center Acknowledgement Dr Hao Li for his excellent

More information

Image Enhancement: Methods. Digital Image Processing. No Explicit definition. Spatial Domain: Frequency Domain:

Image Enhancement: Methods. Digital Image Processing. No Explicit definition. Spatial Domain: Frequency Domain: Image Enhancement: No Explicit definition Methods Spatial Domain: Linear Nonlinear Frequency Domain: Linear Nonlinear 1 Spatial Domain Process,, g x y T f x y 2 For 1 1 neighborhood: Contrast Enhancement/Stretching/Point

More information

Bayesian approach to image reconstruction in photoacoustic tomography

Bayesian approach to image reconstruction in photoacoustic tomography Bayesian approach to image reconstruction in photoacoustic tomography Jenni Tick a, Aki Pulkkinen a, and Tanja Tarvainen a,b a Department of Applied Physics, University of Eastern Finland, P.O. Box 167,

More information

BioE Exam 1 10/9/2018 Answer Sheet - Correct answer is A for all questions. 1. The sagittal plane

BioE Exam 1 10/9/2018 Answer Sheet - Correct answer is A for all questions. 1. The sagittal plane BioE 1330 - Exam 1 10/9/2018 Answer Sheet - Correct answer is A for all questions 1. The sagittal plane A. is perpendicular to the coronal plane. B. is parallel to the top of the head. C. represents a

More information

Phase-shifting coronagraph

Phase-shifting coronagraph Phase-shifting coronagraph François Hénault, Alexis Carlotti, Christophe Vérinaud Institut de Planétologie et d Astrophysique de Grenoble Université Grenoble-Alpes Centre National de la Recherche Scientifique

More information

Image Assessment San Diego, November 2005

Image Assessment San Diego, November 2005 Image Assessment San Diego, November 005 Pawel A. Penczek The University of Texas Houston Medical School Department of Biochemistry and Molecular Biology 6431 Fannin, MSB6.18, Houston, TX 77030, USA phone:

More information

New signal representation based on the fractional Fourier transform: definitions

New signal representation based on the fractional Fourier transform: definitions 2424 J. Opt. Soc. Am. A/Vol. 2, No. /November 995 Mendlovic et al. New signal representation based on the fractional Fourier transform: definitions David Mendlovic, Zeev Zalevsky, Rainer G. Dorsch, and

More information

Technique 1: Volumes by Slicing

Technique 1: Volumes by Slicing Finding Volumes of Solids We have used integrals to find the areas of regions under curves; it may not seem obvious at first, but we can actually use similar methods to find volumes of certain types of

More information

NONLOCAL DIFFUSION EQUATIONS

NONLOCAL DIFFUSION EQUATIONS NONLOCAL DIFFUSION EQUATIONS JULIO D. ROSSI (ALICANTE, SPAIN AND BUENOS AIRES, ARGENTINA) jrossi@dm.uba.ar http://mate.dm.uba.ar/ jrossi 2011 Non-local diffusion. The function J. Let J : R N R, nonnegative,

More information

Restoration of Missing Data in Limited Angle Tomography Based on Helgason- Ludwig Consistency Conditions

Restoration of Missing Data in Limited Angle Tomography Based on Helgason- Ludwig Consistency Conditions Restoration of Missing Data in Limited Angle Tomography Based on Helgason- Ludwig Consistency Conditions Yixing Huang, Oliver Taubmann, Xiaolin Huang, Guenter Lauritsch, Andreas Maier 26.01. 2017 Pattern

More information

Sistemas de Aquisição de Dados. Mestrado Integrado em Eng. Física Tecnológica 2016/17 Aula 3, 3rd September

Sistemas de Aquisição de Dados. Mestrado Integrado em Eng. Física Tecnológica 2016/17 Aula 3, 3rd September Sistemas de Aquisição de Dados Mestrado Integrado em Eng. Física Tecnológica 2016/17 Aula 3, 3rd September The Data Converter Interface Analog Media and Transducers Signal Conditioning Signal Conditioning

More information

Intensity Transformations and Spatial Filtering: WHICH ONE LOOKS BETTER? Intensity Transformations and Spatial Filtering: WHICH ONE LOOKS BETTER?

Intensity Transformations and Spatial Filtering: WHICH ONE LOOKS BETTER? Intensity Transformations and Spatial Filtering: WHICH ONE LOOKS BETTER? : WHICH ONE LOOKS BETTER? 3.1 : WHICH ONE LOOKS BETTER? 3.2 1 Goal: Image enhancement seeks to improve the visual appearance of an image, or convert it to a form suited for analysis by a human or a machine.

More information