2014
DOI: 10.1364/oe.22.002745
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A robust tool for photon source geometry measurements using the fractional Talbot effect

Abstract: Originally published at: Lovric, Goran; Oberta, Peter; Mohacsi, Istvan; Stampanoni, Marco; Mokso, Rajmund (2014). A robust tool for photon source geometry measurements using the fractional Talbot effect. Optics Express, 22(3):2745. DOI: https://doi.org/10.1364/OE.22.002745A robust tool for photon source geometry measurements using the fractional Talbot effect Paul Scherrer Institute, 5232 Villigen, Switzerland *goran.lovric@psi.ch Abstract: A reliable measurement of beam coherence is important for optim… Show more

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Cited by 10 publications
(7 citation statements)
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References 35 publications
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“…Right tibiae were mechanically fixed with wax to prevent sample movement and the tibiofibular junctions were scanned using SR CT at the TOMCAT beamline of the Swiss Light Source at a voxel size of 1.3 μm and 325 nm (with the highest the spatial resolution needed to detect the presence and size of smallest intracortical capillaries) at two different sample-to-detector distances, (15 and 25 mm, for standard X-ray tomography and phase-sensitive imaging respectively,) 33 , 34 (Fig. 1b,c ).…”
Section: Methodsmentioning
confidence: 99%
“…Right tibiae were mechanically fixed with wax to prevent sample movement and the tibiofibular junctions were scanned using SR CT at the TOMCAT beamline of the Swiss Light Source at a voxel size of 1.3 μm and 325 nm (with the highest the spatial resolution needed to detect the presence and size of smallest intracortical capillaries) at two different sample-to-detector distances, (15 and 25 mm, for standard X-ray tomography and phase-sensitive imaging respectively,) 33 , 34 (Fig. 1b,c ).…”
Section: Methodsmentioning
confidence: 99%
“…The sample to detector distance z was set to 100 mm, yielding an optimal trade-off between contrast-to-noise ratio and resolution settings 40 and at the same time keeping the penumbral blurring at a minimum, i.e. with projected X-ray source sizes (full width at half maximum) being 0.51 μm and 0.18 μm in the horizontal and vertical direction, respectively 42 .
Figure 7 Schematic description of the imaging layout ( a ) at the X02DA TOMCAT beamline with the ( b ) complete triggering schematic for the prospective heartbeat-triggered gating technique and ( c ) the final in vivo endstation design with all accompanying components.
…”
Section: Methodsmentioning
confidence: 99%
“…It is difficult to reveal weakly absorbing structures of soft tissues consisting of low‐Z elements (such as C, H, O, N, and so on) due to poor image contrast arisen from soft tissues almost transparent to hard X‐rays. Compared with traditional micro‐CT based on the attenuation effect, the phase sensitive imaging technique generally provides much higher image contrast and lower radiation dose for low‐Z elemental samples . Therefore, X‐ray phase‐contrast imaging (XPCI) enables us to observe inner weakly absorbing structures with high phase sensitivity, particularly suitable for visualizing and quantifying fine electron density differences of biomedical structural information with sufficient image contrast.…”
Section: Introductionmentioning
confidence: 99%
“…image contrast and lower radiation dose for low-Z elemental samples. [4][5][6] Therefore, X-ray phase-contrast imaging (XPCI) enables us to observe inner weakly absorbing structures with high phase sensitivity, particularly suitable for visualizing and quantifying fine electron density differences of biomedical structural information with sufficient image contrast. In recent years, many XPCI techniques, including crystal interferometry, analyzer-based imaging, grating-based imaging, and propagation-based imaging, have been proposed and developed to improve hard X-ray image contrast through translating the phase shift into the accessibly recorded intensity variations.…”
Section: Introductionmentioning
confidence: 99%