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Image Reconstruction. Atam P Dhawan. y. b. Radiating Object f( a,b,g ). Image g(x,y,z). Image Formation System h. g. z. Image Domain. Object Domain. x. a. Image Formation. b. y. Radiating Object. Image. Image Formation System h. Selected Cross-Section. g. z.
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Image Reconstruction Atam P Dhawan
y b Radiating Object f(a,b,g) Image g(x,y,z) Image Formation System h g z Image Domain Object Domain x a Image Formation
b y Radiating Object Image Image Formation System h Selected Cross-Section g z Image Domain Object Domain x a Radiation Source Reconstructed Cross-Sectional Image Image Formation: External Source
b y Image Radiating Object Image Formation System h Selected Cross-Section g z Image Domain Object Domain x a Reconstructed Cross-Sectional Image Image Formation: Internal Source
y q p f(x,y) q x p P(p,q) q Line integral projection P(p,q) of the two-dimensional Radon transform. Radon Transform
Projection p1 A Reconstruction Space B Projection p3 Projection p2 Radon Transform
Fourier Slice Theorem • X-y coordinate system rotated to p-q u = w cos q v= w sin q
v Sqk(w) Sq2(w) F(u,v) Sq1(w) qk q2 q1 u Fourier Slice Theorem…
Filtered Backprojection The integration over the spatial frequency variable w should be carried out from But in practice, the projections are considered to be bandlimited. This means that any spectral energy beyond a spatial frequency, say W, must be ignored. can be computed as in the spatial domain and is bandlimited. is the Fourier transform of the filter kernel function
in the spatial domain and is bandlimited. is the Fourier transform of the filter kernel function
H(w) 1/2t -1/2t 1/2t w
If the projections are sampled with a time interval of t, the projections can be represented as Using the Sampling theorem and the bandlimited constraint, all spatial frequency components beyond W are ignored such that For the bandlimited projections with a sampling interval of t
h(t) hR-L(p) t HHamming(p) H(w) w -1/2t 1/2t Filter Function
f1 f2 f3 Overlapping area for defining wi,j Ray with ray sum pi fN Iterative ART
Reconstruction in MRI Fourier Transform Reconstruction Method