Ultrasound Computed Tomography

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Presentation transcript:

Ultrasound Computed Tomography 何祚明 陳彥甫 2002/05/15

Introduction Conventional X-ray image is the superposition of all the planes normal to the direction of propagation. The tomography image is effectively an image of a slice taken through a 3-D volume. A B

Clinical application Problems of X-ray Mammography An estimated 10-15% of breast cancers evade detection by mammography Poor differentiation of malignant tumors from highly common cysts (while ultrasound can do so with accuracies of 90-100%) UCT can provide not only structural/density information, but also tissue compressibility and speed of sound maps

Tomography Time of flight or intensity attenuation Array transducer : 1-D data (only tf) Rotation : 2-D data (tf on range and angle q) Scan : 3-D data (y position, tf and angle q)

Tomography reconstruct A R q

Reconstruct method Iterative method Direct reconstruction Algebraic Reconstruction Technique (ART) Direct reconstruction Fourier transform Alternative direct reconstruction Back projection

Central Section Theorem y y x g90(y) f(x,y)

Ambiguity angle q R q y r q x f(x,y) xcosq + ysinq = R

Equations 1D FT of projection function

Cont’d 2D Fourier transform (u,v) in polar coordinates is (rcosq, rsinq) 2 D inverse Fourier Transform

figures gq(R) R y v r Gq(r) q q x u f(x,y)

Tomography u v F(u,v) F{g(y)} u v ρ q u v ρ Fourier Transform of Projection at q, F(r,q)=F1{gq(R)} In polar coordinates F(u,v)=F(r, q)

Algorithm summation The Fourier transform of a projection at angle q forms a line in the 2-D Fourier plane at this same angle. After filling the entire plane F(r, q) with the transforms of the projections at all angles, the reconstructed density is provided by the two-dimensional inverse transform. 1. 1D FT each of the projections gq(R) Gq(r) 2. Interpolate F(r,q) to F(u,v) solve coordinate problems (polar to rectangular coordinates) 3. Inverse 2D FT Gq(r)  F(x, y)

Simulation method Finite small point Gaussian envelope to time-of-flight gq(R) FFT and phase compensation For loops for Integration

Results I. Time of flight spectrum original data g(r,thita) 0.8 50 0.6 100 0.4 0.2 150 20 40 60 80

Results II.

Experiment architecture y Transducer Phantom Transducer Water Tank

Future works Experimental data acquisition Other correct reconstruction algorithm ART, Fourier Transform Back propagation

Patent Map 年代/公司別 Siemens U.S.Surgical 3rd Party Westinghouse GE Philips 1978 核心專利 4,105,018 (Greenleaf) 1981 4,279,157 (Australia) 4,509,368 1985 4,549,265 4,829,430 1989 (Greenleaf) 5,047,931 1991 (EG&G) 5,181,778 1993 1994 5,318,028 1995 5,433,206 5,433,202 (Elscint) 5,513,236 1996 5,603,326 5,663,995 1997 (Northrop) 5,841,890 1998 1999 5,938,613 5,983,123 2000 6,027,457 2001 6,324,241

Patent Map Method/ Process Device/ Apparatus System 合計 17 11 7 35

Patent Analysis James F. Greenleaf : measurement of the time-of-flight of acoustic signal ; reducing artifacts… Westinghouse : array scanner providing electronic scanning GE : helical or spiral scan, 3D reconstruction

Patent Analysis Northrop Grumman : Multi-dimensional wavelet tomography (using wavelet decomposition upon the projection image) U.S.Surgical : combines mammography equipment (X-ray) with an ultrasonic transducer

Core Patent 1985, The Commonwealth of Australia Ultrasound tomography, the apparatus comprising paired couples of transmission transducers and reflection transducers, the paired couples of transducer means being independently operable within a container of ultrasound transmission medium….

Core Technique Pulses of acoustic energy are transmitted from a plurality of different directions through a plane of interest of a body to be examined. Time-of-flight of the pulses is measured for individual paths through the body, and from the data thus obtained the spatial distribution of the acoustic velocity through the plane or planes within the body is reconstructed using a mathematical reconstruction technique.

Central Section Theorem 2D Fourier transform Central Section Theorem