2011
DOI: 10.1143/apex.4.066603
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X-ray Phase Imaging Using Lau Effect

Abstract: X-ray phase imaging based on the Lau effect is demonstrated with an incoherent laboratory X-ray source. Its optical configuration resembles the inverse geometry of the X-ray Talbot–Lau interferometer, which employs a large-area amplitude grating. However, the proposed approach avoids the use and hence fabrication difficulty of such a grating, which is advantageous when constructing an X-ray phase imaging apparatus. With a Mo-target source, differential phase images of polymer spheres were successfully obtained… Show more

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Cited by 66 publications
(61 citation statements)
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“…20,[22][23][24][25][26] Moreover, the formulas for the 1-D phase grating interferometry can easily be derived from the general twodimensional theory through a dimension reduction. As is shown in Fig.…”
Section: Methodsmentioning
confidence: 99%
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“…20,[22][23][24][25][26] Moreover, the formulas for the 1-D phase grating interferometry can easily be derived from the general twodimensional theory through a dimension reduction. As is shown in Fig.…”
Section: Methodsmentioning
confidence: 99%
“…(20) and (21) dictate that a large SID must be used for matching a fractional Talbot distance. 20,21 For example, for a 20-keV x-ray interferometer based on a 2-D checkerboard phase grating of 5-µm period, in order to achieve a magnification factor of 15, Eqs. (20) and (21) dictate that the most compact geometry should set R 1 = 10.8 cm and R 2 = 151.2 cm, so SID = 1.62 m. For sake of convenience in discussion, let us call this geometry as interferometer-configuration (20) and (21)] for 20 keV x-rays, it will not match such Talbot-distance matching equations for a polychromatic beam with an average energy of 20 keV.…”
Section: -15mentioning
confidence: 99%
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“…This can be achieved by reducing the targets-G 1 distance, since the magnification is proportional to the targetdetector distance divided by the targets-G 1 distance. This configuration was originally proposed by Momose et al, but the source-detector distance was more than 7 m in their experimental setup [5] because of the long G 0 -G 1 distance of 19 cm required to preserve coherence of the x-rays at G 1 . In this study, we discuss a compact interferometer using a single transmission grating, where the source-detector distance was within 1 m, and multiline embedded targets of 1 μm line width were used as the x-ray sources.…”
mentioning
confidence: 99%