P. Gerlach
University of Wuppertal
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Publication
Featured researches published by P. Gerlach.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
I. Gorelov; Grant Gorfine; M. R. Hoeferkamp; S. Seidel; A. Ciocio; K. Einsweiler; M. Gilchriese; A Joshi; S. Kleinfelder; R. Marchesini; O Milgrome; N Palaio; F Pengg; J. Richardson; G. Zizka; M. Ackers; P. Fischer; M. Keil; S. Meuser; T. Stockmanns; J. Treis; N. Wermes; C. Gößling; F. Hügging; J. Wüstenfeld; R. Wunstorf; Dario Barberis; R. Beccherle; M. Cervetto; Giovanni Darbo
Silicon pixel sensors developed by the ATLAS collaboration to meet LHC requirements and to withstand hadronic irradiation to fluences of up to
arXiv: Instrumentation and Detectors | 2005
Kendall Reeves; J. Schultes; J Richter; Jörn Grosse-Knetter; T. Flick; S. Kersten; F Huegging; M Imhaeuser; J. Weingarten; P. Gerlach; I Rottlaender; P. Mättig; J Schumacher; Norbert Wermes; P. Kind; K. H. Becks; K. Lantzsch
10^{15} n_eq/cm^{2}
Journal of Instrumentation | 2007
T. Flick; P. Gerlach; Kendall Reeves; P. Mättig
have been evaluated using a test beam facility at CERN providing a magnetic field. The Lorentz angle was measured and found to alter from 9.0 deg. before irradiation, when the detectors operated at 150 V bias at B=1.48 T, to 3.1 deg after irradiation and operating at 600 V bias at 1.01 T. In addition to the effect due to magnetic field variation, this change is explained by the variation of the electric field inside the detectors arising from the different bias conditions. The depletion depths of irradiated sensors at various bias voltages were also measured. At 600 V bias 280 micron thick sensors depleted to ~200 micron after irradiation at the design fluence of 1 10^{15} 1 MeV n_eq/cm2 and were almost fully depleted at a fluence of 0.5 * 10^{15} 1 MeV n_eq/cm2. The spatial resolution was measured for angles of incidence between 0 deg and 30 deg. The optimal value was found to be better than 5.3 micron before irradiation and 7.4 micron after irradiation.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
K. H. Becks; P. Gerlach; C. Grah; P. Mättig; T. Rohe
The innermost part of the ATLAS (A Toroidal LHC ApparatuS)[1] experiment at the LHC (Large Hadron Collider) will be a pixel detector, which is presently under construction. Once installed into the experimental area, access will be extremely limited. To ensure that the integrated detector assembly operates as expected, a fraction of the detector which includes the power supplies and monitoring system, the optical readout, and the pixel modules themselves, has been assembled and operated in a laboratory setting for what we refer to as system tests. Results from these tests are presented.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
T. Flick; K. H. Becks; P. Gerlach; S. Kersten; P. Mättig; Simon Nderitu Kirichu; Kendall Reeves; Jennifer Richter; J. Schultes
As with all detector systems at the Large Hadron Collider (LHC), the assignment of data to the correct bunch crossing, where bunch crossings will be separated in time by 25 ns, is one of the challenges for the ATLAS pixel detector. This document explains how the detector system will accomplish this by describing the general strategy, its implementation, the optimisation of the parameters, and the results obtained during a combined testbeam of all ATLAS subdetectors.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
K. H. Becks; P. Gerlach; Karl-Walter Glitza; Pascal Knebel; P. Mättig; Bernd Sanny; Sebastian Reuschel; Swetlana Springer; Bernd Witt
The Multi-Chip-Module-Deposited (MCM-D) technique has been used to build hybrid pixel detector assemblies. This paper summarises the results of an analysis of data obtained in a test beam campaign at CERN. Here, single chip hybrids made of ATLAS pixel prototype read-out electronics and special sensor tiles were used. They were prepared by the Fraunhofer Institut fuer Zuverlaessigkeit und Mikrointegration, IZM, Berlin, Germany. The sensors feature an optimized sensor geometry called equal sized bricked. This design enhances the spatial resolution for double hits in the long direction of the sensor cells.