Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where P. Gerlach is active.

Publication


Featured researches published by P. Gerlach.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002

A measurement of Lorentz angle and spatial resolution of radiation hard silicon pixel sensors

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

System Tests of the ATLAS Pixel Detector

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

ATLAS pixel detector timing optimisation with the back of crate card of the optical pixel readout system

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

Test beam results of geometry optimized hybrid pixel detectors

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

Optical readout in a multi-module system test for the ATLAS pixel detector

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

Local support assembly of the ATLAS pixel detector

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.

Collaboration


Dive into the P. Gerlach's collaboration.

Top Co-Authors

Avatar

K. H. Becks

University of Wuppertal

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar

P. Mättig

Weizmann Institute of Science

View shared research outputs
Top Co-Authors

Avatar

T. Flick

University of Wuppertal

View shared research outputs
Top Co-Authors

Avatar

J. Schultes

University of Wuppertal

View shared research outputs
Top Co-Authors

Avatar

S. Kersten

University of Wuppertal

View shared research outputs
Top Co-Authors

Avatar

P. Mättig

Weizmann Institute of Science

View shared research outputs
Top Co-Authors

Avatar

C. Gößling

Technical University of Dortmund

View shared research outputs
Top Co-Authors

Avatar

F Huegging

University of Wuppertal

View shared research outputs
Top Co-Authors

Avatar

F. Hügging

Technical University of Dortmund

View shared research outputs
Researchain Logo
Decentralizing Knowledge