M. Schaeffer
Delphi Automotive
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by M. Schaeffer.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
N. Bingefors; H. Borner; R. Boulter; M. Caccia; V. Chabaud; H. Dijkstra; P. Eerola; E. Gross; R. Horisberger; L. Hubbeling; B. Hyams; M. Karlsson; G. Maehlum; K. Ratz; I. Roditi; J. Straver; W. Trischuk; P. Weilhammer; Y. Dufour; P. Bruckman; Pawel Jalocha; P. Kapusta; M. Turala; A. Zalewska; J. Lindgren; R. Orava; K. Osterberg; C. Ronnqvist; H. Saarikko; J.P. Saarikko
The DELPHI Microvertex detector, which has been in operation since the start of the 1990 LEP run, consists of three layers of silicon microstrip detectors at average radii of 6.3, 9.0 and 11.0 cm. The 73728 readout strips, oriented along the beam, have a total active area of 0.42 m2. The strip pitch is 25 μm and every other strip is read out by low power charge amplifiers, giving a signal to noise ratio of 15:1 for minimum ionizing particles. On-line zero suppression results in an average data size of 4 kbyte for Z0 events. After a mechanical survey and an alignment with tracks, the impact parameter uncertainty as determined from hadronic Z0 decays is well described by (69pt)2 + 242 μm, with pt in GeV/c. For the 45 GeV/c tracks from Z0 → μ− decays we find an uncertainty of 21 μm for the impact parameter, which corresponds to a precision of 8 μm per point. The stability during the run is monitored using light spots and capacitive probes. An analysis of tracks through sector overlaps provides an additional check of the stability. The same analysis also results in a value of 6 μm for the intrinsic precision of the detector.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1994
A. Holmes-Siedle; M. Robbins; S. Watts; Phillip Allport; R. Brenner; H.G. Moser; S. Roe; J. Straver; Peter Weilhammer; P. Chochula; I. Mikulec; S. Moszczynski; M. Turala; W. Dabrowski; P. Grybos; M. Idzik; D. Loukas; K. Misiakos; I. Siotis; K. Zachariadou; W. Dulinski; J. Michele; M. Schaeffer; R. Turchetta; P.S.L. Booth; J. Richardson; N.A. Smith; K. Gill; G. Hall; R. Sachdeva
Abstract The RD20 collaboration is investigating the design and operation of an LHC inner tracking detector based on silicon microstrips. Measurements have been made on prototype detectors after irradiation with electrons, neutrons, photons, and protons for doses up to 5 Mrad and fluences up to 10 15 particles/cm 2 . The annealing of effective doping changes caused by high neutron fluences, one of the major limits to detector lifetime at the LHC, is shown to be strongly inhibited by cooling below room temperature. Detailed results are presented on the critical issue of microstrip capacitance. We have also investigated bulk damage caused by high-energy protons, interstrip isolation after neutron irradiation, and MOS capacitors irradiated with electrons and photons.
ieee nuclear science symposium | 1990
E.G. Anassontzis; P. Ioannou; G. Kalkanis; S. Katsanevas; I. Kontaxis; C. Koukoumelis; S. Nounos; P. Preve; L.K. Resvanis; J.M. Brunet; J. Dolbeau; L. Guglielmi; F. Ledroit; D. Poutot; G. Tristram; P. Baillon; M. Barranco-Luque; M. Davenport; S. Delorme; J. Dixon; M. Dracos; D. Fraissard; J.B. Franco; E. Gaumann; B. Goret; F. Hahn; S. Haider; W. Klempt; B. Koene; G. Lecoeur
The DELPHI detector installed in the LEP (Large Electron-Positron Collider) is equipped with RICH (ring imaging Cherenkov) counters. The barrel part incorporates a liquid (C/sub 6/F/sub 14/) and a gaseous (C/sub 5/F/sub 12/) radiator, providing particle identification up to 20 GeV/c. The Cherenkov photons of both radiators are detected by TPC (time projection chamber)-like photon detectors. The drift gas (75% CH/sub 4/+25% C/sub 2/H/sub 6/) is doped with TMAE (tetrakis-dimethylamine-ethylene) by which the ultraviolet Cherenkov photons are converted into single free photoelectrons. These are drifted towards multiwire proportional chambers at the end of the drift tubes, and the space coordinates of the conversion point are determined. One half of the barrel RICH is now equipped with drift tubes and has provided results from the liquid radiator since spring 1990. The gas radiator has been tested with C/sub 2/F/sub 6/ as a preliminary filling since August 1990. The data obtained demonstrate the good particle identification potential. For the liquid radiator, the number of detected photons per ring in hadron jets is N=8, whereas for muon pairs (single tracks) N=10 has been obtained. For the gas radiator, 2.1 photons per track were observed, which demonstrates good functioning of the focussing mirrors. >
Proceedings of the 26th International Conference on High Energy Physics | 2008
M. Caccia; H. Borner; V. Chabaud; H. Dijkstra; P. Eerola; E. Gross; B. Hyams; R. Horisberger; L. Hubbeling; Magnus Karlsson; G. Maehlum; I. Roditi; J. Straver; W. Trischuk; P. Weilhammer; Y. Dufour; P. Bruckman; P. Jal; ocha; P. Kapusta; M. Tural; A. Zalewska; J. Lindgren; R. Orava; K. Osterberg; C. Ronnqvist; H. Saarikko; J.P. Saarikko; T. Tuuva; B. d’Almagne
The main characteristics of the DELPHI Microvertex Detector are presented. The performance in terms of impact parameter resolution, association efficiency, and ambiguity is evaluated after two years of data taking at LEP.
AIP Conference Proceedings (American Institute of Physics); (United States) | 1992
M. Caccia; H. Borner; V. Chabaud; H. Dijkstra; P. Eerola; E. Gross; B. Hyams; R. Horisberger; L. Hubbeling; Magnus Karlsson; G. Maehlum; I. Roditi; J. Straver; W. Trischuk; P. Weilhammer; Y. Dufour; P. Bruckman; Pawel Jalocha; P. Kapusta; M. Turala; A. Zalewska; J. Lindgren; R. Orava; K. Osterberg; C. Ronnqvist; H. Saarikko; J.P. Saarikko; T. Tuuva; B. D'Almagne; P. Bambade