2019
DOI: 10.1002/mp.13957
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The trigonometric orthogonality of phase‐stepping curves in grating‐based x‐ray phase‐contrast imaging: Integral property and its implications for noise optimization

Abstract: Purpose Grating‐based x‐ray phase‐contrast imaging (GPCI) is a promising technique for clinical applications as it can provide two newly emerging imaging modalities (differential phase‐contrast and dark‐field contrast) in addition to the conventional absorption contrast. As far, phase‐stepping strategy is the most commonly used approach in GPCI to indirectly acquire differential phase‐contrast and dark‐field contrast. It is known that the obtained phase‐stepping curves (PSCs) have the cosine property and the c… Show more

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Cited by 4 publications
(6 citation statements)
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References 30 publications
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“…To overcome these limitations of the original deconvolution‐based MMA (named DB‐MMA in this paper), some analytic MMA methods are developed recently 18,19 . The first one is referred as the direct MMA (D‐MMA) 18 that is applicable to EI and ABI at first, and it is extended to the GBI with some preprocessing operations 23 .…”
Section: Methodsmentioning
confidence: 99%
See 4 more Smart Citations
“…To overcome these limitations of the original deconvolution‐based MMA (named DB‐MMA in this paper), some analytic MMA methods are developed recently 18,19 . The first one is referred as the direct MMA (D‐MMA) 18 that is applicable to EI and ABI at first, and it is extended to the GBI with some preprocessing operations 23 .…”
Section: Methodsmentioning
confidence: 99%
“…The first one is referred as the direct MMA (D‐MMA) 18 that is applicable to EI and ABI at first, and it is extended to the GBI with some preprocessing operations 23 . Then, a generalized D‐MMA (GD‐MMA) is developed by using the trigonometric orthogonality of PSCs, 19 which can be utilized to improve the noise performance of the original D‐MMA. The typical contrasts retrieved by D‐MMA and GD‐MMA can be expressed as: AM0false(gfalse)=ππgfalse(ϕfalse)dϕ=ππsfalse(ϕfalse)dϕππffalse(ϕfalse)dϕ, truerightPM¯1(g)=leftM1(g)M0(g)=ππϕ·g(ϕ)dϕππg(ϕ)dϕ=leftππh1(ϕ)·s(ϕ)dϕππs(ϕ)dϕππh1(ϕ)·f(ϕ)dϕππf(ϕ)dϕ, truerightDM2(g)=…”
Section: Methodsmentioning
confidence: 99%
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