Computed Tomography: Algorithms, Insight, and Just Enough Theory 2021
DOI: 10.1137/1.9781611976670.ch14
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Chapter 14: Looking Ahead

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Cited by 12 publications
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“…Underdetermined linear system. Consider a small scale CT problem [10] of the form b " Ax `e, where the true signal x P R 100ˆ100 is the Shepp-Logan phantom and the noise satisfies e " N p0, λ ´1I q with λ " 10. Furthermore, the forward operator A is a discretized Radon transform at 20 equally spaced angles from 0 to 180 degrees with 120 rays per angle and using parallel-beam geometry.…”
Section: Gibbs Samplermentioning
confidence: 99%
“…Underdetermined linear system. Consider a small scale CT problem [10] of the form b " Ax `e, where the true signal x P R 100ˆ100 is the Shepp-Logan phantom and the noise satisfies e " N p0, λ ´1I q with λ " 10. Furthermore, the forward operator A is a discretized Radon transform at 20 equally spaced angles from 0 to 180 degrees with 120 rays per angle and using parallel-beam geometry.…”
Section: Gibbs Samplermentioning
confidence: 99%
“…Projections are recorded at different angles around the object. By modelling attenuation using the Beer-Lambert law with line integrals [7], we can formulate a discretized linear inverse problem b = Au + e.…”
Section: The Inverse Problem Of Computed Tomographymentioning
confidence: 99%
“…A ∈ R n×m is the system matrix where the entry A i,j describes the intersection length of the i'th x-ray with the j'th pixel. For more details on the general CT inverse problem see [7], for example, for a motivation of the form of (1), which arises from the Beer-Lambert law of x-ray attenuation in matter combined with a postlogarithm Gaussian approximation to the general Poisson noise model for transmission CT.…”
Section: The Inverse Problem Of Computed Tomographymentioning
confidence: 99%
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