2005
DOI: 10.1016/j.cocis.2004.10.004
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Applications of synchrotron radiation micro-focus techniques to the study of polymer and biopolymer fibers

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Cited by 53 publications
(41 citation statements)
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“…The ID13 beamline is characterized by a 18 mm period in-vacuum undulator optimized for 13 keV and the optical setup for a ͑sub͒micrometer beam ͑variable in a region from 0.5 to 5 m͒ is defined by a Kirkpatrick-Baez mirror. 17 The radiation wavelength was 0.9755 Å and a 16 bit readout MARCCD ͑Mar Inc., U.S.͒ detector with an x-ray converter screen of 130 mm diameter and 2048ϫ 2048 pixels with a pixel size of 64.45ϫ 64.45 m 2 was used for recording the diffraction patterns. For faster readout, data were recorded in binning mode with 512ϫ 512 pixels.…”
Section: Methodsmentioning
confidence: 99%
“…The ID13 beamline is characterized by a 18 mm period in-vacuum undulator optimized for 13 keV and the optical setup for a ͑sub͒micrometer beam ͑variable in a region from 0.5 to 5 m͒ is defined by a Kirkpatrick-Baez mirror. 17 The radiation wavelength was 0.9755 Å and a 16 bit readout MARCCD ͑Mar Inc., U.S.͒ detector with an x-ray converter screen of 130 mm diameter and 2048ϫ 2048 pixels with a pixel size of 64.45ϫ 64.45 m 2 was used for recording the diffraction patterns. For faster readout, data were recorded in binning mode with 512ϫ 512 pixels.…”
Section: Methodsmentioning
confidence: 99%
“…48,49 Other possibilities to cope with radiation damage are very fast measurements, which have become feasible with new developments of pixel detectors 50 in combination with scanning. 11,13 Due to the diffusion of radicals ͑the mean diffusion distance in water is in the order of several m / s at room temperature 51 ͒, there are also limits to this. Staying ahead of radiation damage requires therefore essentially much faster scanning as compared to now, which is, in principle, feasible with increased flux density and faster detectors.…”
Section: Radiation Damagementioning
confidence: 99%
“…While in a typical laboratory setup, D cannot be made much smaller than about 100 m for primary intensity reasons, 9 synchrotron radiation allows readily to obtain beam sizes down to 10 m at bending magnet and wiggler sources 30,35,36 and down to 1 m at undulator sources at dedicated high energy x-ray facilities such as the ESRF. 11,13 Even though much smaller beam sizes have recently been demonstrated with hard x rays, [37][38][39] The SAXS/ WAXS area detector is placed in the y-z plane at a distance L behind the specimen. The scattered intensity in polar detector coordinates I͑r , ͒ is converted into reciprocal space units I͑q , ͒, where the length of the scattering vector q is given by q =4 sin / , with 2 = arctan͑r / L͒ being the scattering angle and the x-ray wavelength.…”
Section: A Experimental Setupmentioning
confidence: 99%
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“…The single-fiber experiments have been carried out at the microfocus beamline ID13 at ESRF, Grenoble [31]. A 12.7 keV X-ray beam was focused with a pair of short focal length Kirkpatrick Baez (KB) mirrors [32] to a 7 μm spot at the sample.…”
Section: Experimental Scattering Functionmentioning
confidence: 99%