1998
DOI: 10.1016/s0168-9002(98)00223-x
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Study and application of hole structures as gas gain devices for two dimensional high rate X-ray detectors

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Cited by 38 publications
(22 citation statements)
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“…The copper-clad bottom side of the GEM shields all currents induced by charge movements appearing above this electrode; especially the slow ions do not contribute to the signal shape, which is, however, the case for micromegas or MicroCAT detectors [24,25]. The crucial parameters for the width t w of the box-shaped current are the electron drift velocity v e in the electric field of the induction region and the distance d between the bottom side of the GEM and the anode which amounts to 1 mm in our case:…”
Section: Signal Length Investigationsmentioning
confidence: 99%
“…The copper-clad bottom side of the GEM shields all currents induced by charge movements appearing above this electrode; especially the slow ions do not contribute to the signal shape, which is, however, the case for micromegas or MicroCAT detectors [24,25]. The crucial parameters for the width t w of the box-shaped current are the electron drift velocity v e in the electric field of the induction region and the distance d between the bottom side of the GEM and the anode which amounts to 1 mm in our case:…”
Section: Signal Length Investigationsmentioning
confidence: 99%
“…1 The small increase in counter-gas pressure from 2 to 2.5 Bar (that is in comparison with the breadboard instrument) will tend to offset this improvement as shown in pressure vs. resolution evaluations done for hole-structures. 10 For our application, good energy resolution is useful in maintaining image contrast, but not critical.…”
Section: The Electron Cloudmentioning
confidence: 99%
“…A detailed description of the detector has already been presented in earlier works (see Besch et al, 1997;Sarvestani et al, 1998a). Here, only the main features are brie¯y summarized.…”
Section: Detector Set-upmentioning
confidence: 99%
“…During this process primary charge is generated. In the constant drift ®eld (24 mm length) the ions are transported to the drift cathode, while the electrons are transported to the gas gain structure (MicroCAT; see Sarvestani et al, 1998a). The MicroCAT (supplied by Koenen Siebdrucktechnik, 85521 Ottobrunn, Germany) consists of a 55 mm-thick nickel foil perforated with microholes (116 mm diameter) in a hexagonal arrangement with a pitch of 164 mm.…”
Section: Detector Set-upmentioning
confidence: 99%