1988
DOI: 10.1016/0168-9002(88)90450-0
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PDA system for energy dispersive EXAFS

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Cited by 38 publications
(9 citation statements)
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“…Two types of photodiode array (PDA) detectors have been used with some success: (1) directly exposed X-ray PDAs and (2) phosphor scintillators coupled to PDAs to convert X-ray photons to visible photons . The first type has a higher gain than the second one 71 but has a narrower detectable X-ray energy range (2−20 keV) and suffers radiation damage resulting in a permanent rise in dark count noise and a decrease in sensitivity.…”
Section: Linear Position-sensitive Detectorsmentioning
confidence: 99%
“…Two types of photodiode array (PDA) detectors have been used with some success: (1) directly exposed X-ray PDAs and (2) phosphor scintillators coupled to PDAs to convert X-ray photons to visible photons . The first type has a higher gain than the second one 71 but has a narrower detectable X-ray energy range (2−20 keV) and suffers radiation damage resulting in a permanent rise in dark count noise and a decrease in sensitivity.…”
Section: Linear Position-sensitive Detectorsmentioning
confidence: 99%
“…Starting from the pioneering work of Matsushita et al (Matsushita & Kaminaga, 1980), the parallel energy acquisition mode (dispersive mode, or D-XAS) has been further developed at the different synchrotron radiation facilities (Phizackerley et al, 1983;Flank et al, 1983;Allinson et al, 1988;Hagelstein et al, 1989;D'Acapito et al, 1992;Allen et al, 1992;Lee et al, 1994) and extensively exploited in different scienti®c domains, from chemistry to biology to solid-state physics (for a review see Fontaine et al, 1989, and references therein).…”
Section: Introductionmentioning
confidence: 99%
“…This is particularly important for, for example, high-pressure studies in a diamond-anvil cell in which the X-rays must pass through an aperture only a few hundred ~m in diameter and for studies of photoexcited states where high excitation power density is necessary. The most commonly employed technique for achieving a desired bend on a crystal has been to apply a force to the apex of a triangular crystal which is held fixed at its base (Phizackerley, Rek, Stephenson, Conradson, Hodgson, Matsushita & Oyanagi, 1983;Dartyge, Depautex, Dubuisson, Fontaine, Jucha, Leboucher & Tourillon, 1986;Allinson, Baker, Greaves & Nicoll, 1988;Hagelstein, Cunis, Frahm, Niemann & Rabe, 1989;Batterman & Berman, 1983). The resulting cylindrical bend, however, produces a broadening of the polychromatic focus spot, which is proportional to the square of the illuminated length of the crystal (Ice & Sparks, 1984).…”
Section: Introductionmentioning
confidence: 99%