L. Gosset
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Featured researches published by L. Gosset.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
G. Barr; C. Bruschini; C. Bocquet; P. Buchholz; D. Cundy; N. Doble; W. Funk; L. Gatignon; A. Gonidec; B. Hallgren; G. Kesseler; A. Lacourt; G. Laverrière; G. Linser; M. Martini; A. Norton; D. Schinzel; W. Seidl; Marco S. Sozzi; H. Taureg; O. Vossnack; H. Wahl; P. Wertelaers; J. Weterings; M. Ziolkowski; A. M. Kalinin; V. Kekelidze; Yu. Kozhevnikov; L. Bertolotto; V. Carassiti
The NA48 collaboration is preparing a new experiment at CERN aiming to study CP violation in the K0-K0 system with an accuracy of 2 × 10−4 in the parameter Re(ϵ′/ϵ). Decays in two π0s will be recorded by a quasi-homogeneous liquid krypton calorimeter. A liquid krypton calorimeter has been chosen to combine good energy, position and time resolution with precise charge calibration and long-term stability. The prototype calorimeter incorporating the final design of the electrode read-out structure is presented in this paper. An energy resolution of ≃3.5%√E with a constant term smaller than 0.5% has been obtained. The time resolution was found to be better than 300 ps above 15 GeV.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1997
R. Aleksan; L. Amerman; D. Aston; M. Benkebil; P. Besson; G. R. Bonneaud; P. Bourgeois; D. N. Brown; J. Chauveau; A. Ciocio; R. Cizeron; A. de Lesquen; L. Del Buono; S. Emery; A. Gaidot; L. Gosset; Daniel E. Hale; G. Hamel de Monchenault; O. Hamon; C. Hearty; A Jouenne; J. Kadyk; H. Kawahara; H. Krueger; G. W. London; M. Long; A. Lu; A. M. Lutz; G. Lynch; D. McShurley
Abstract The principles of the DiRC ring imaging Cherenkov technique are briefly explained and its choice for the B a B ar detector particle identification system is motivated. A large scale prototype of the DIRC for the B a B ar experiment is then described. Details of the design of this prototype and its test in a hadronic particle beam at the CERN-PS are presented, and results from various prototype and test configurations are given. For example, after correcting for geometrical acceptance and estimated collection effects, the number of photoelectrons was measured to be 146 ± 1.8 ± 9 cm −1 , for a track angle of 20° at zero photon transmission distance. The effective attenuation loss was measured to be 4.1 ± 0.7% per meter of bar length, and the observed single photon resolution was 10.0 ± 0.2 mrad. This performance is consistent with what was expected from earlier tests and Monte Carlo simulations, and will be fully adequate for the physics demands of the B a B ar experiment.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1995
D. Bederede; J.B. Cheze; M. De Beer; P. Debu; D. Durand; S. Edard; L. Gosset; J. Heitzmann; F. Louis; E. Mazzucato; A. Migliori; B. Peyaud; S. Schanne; O Steinkamp; G. Tarte; R. Turlay; B. Vallage
We discuss construction details of large drift chambers for the NA48 experiment at CERN. Preliminary measurements on their performance are also presented.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992
B. Aubert; A. Bazan; B. Beaugiraud; J. Colas; T. Leflour; M. Maire; J.P. Vialle; I. Wingerter-Seez; Y. Zolnierowski; Howard Gordon; V. Radeka; D. Rahm; D. Stephani; J.L. Chevalley; Christian Fabjan; D. Fournier; A. Franz; O. Gildemeister; P. Jenni; Marzio Nessi; F. Nessi-Tedaldi; M. Pepe; W. Richter; J. Soderqvist; J.M. Baze; L. Gosset; P. Lavocat; J.P. Lottin; B. Mansoulie; J. Meyer
Abstract A prototype lead-liquid-argon electromagnetic calorimeter with parallel plates and Accordion geometry has been equipped with high speed readout electronics and tested with electron and muon beams at the CERN SPS. For a response peaking time of about 35 ns, fast enough for operation at the future hadron colliders, the energy resolution for electrons is 9.6%/√E[GeV] with a local constant term of 0.3% and a noise contribution of 0.33 E[ GeV ] . The spatial accuracy achieved with a detector granularity of 2.7 cm is 3.7 mm E[ GeV ] and the angular resolution 12 mrad at 60 GeV.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
B. Aubert; A. Bazan; B. Beaugiraud; J. Colas; T. Leflour; M. Maire; J.P. Vialle; I. Wingerter-Seez; Y. Zolnierowski; Howard Gordon; V. Radeka; D. Rahm; D. Stephani; N. Bulgakov; J.L. Chevalley; Christian Fabjan; D. Fournier; O. Gildemeister; P. Jenni; Marzio Nessi; F. Nessi-Tedaldi; M. Pepe; W. Richter; J. Soderqvist; V. Vuillemin; J.M. Baze; L. Gosset; P. Lavocat; J.P. Lottin; B. Mansoulie
Abstract A prototype liquid argon preshower detector with a strip granularity of 2.5 mm has been tested at the CERN SPS in front of a liquid argon Accordion calorimeter. For charged tracks a signal-to-noise ratio of 9.4 and a space resolution of 340 μm were measured; the rejection power against overlapping photons produced in the decay of 50 GeV π 0 s is larger than 3; the precision on
IEEE Transactions on Nuclear Science | 1998
I. Adam; R. Aleksan; D. Aston; P. Bailly; C. Beigbeder; M. Benayoun; M. Benkebil; G. R. Bonneaud; D. Breton; H. Briand; D. N. Brown; P. Bourgeois; J. Chauveau; R. Cizeron; J. Cohen-Tanugi; M. R. Convery; P. David; C de la Vaissiere; A. de Lesquen; L. Del Buono; G. Fouque; A. Gaidot; E. Gastaldi; J.F. Genat; L. Gosset; Daniel E. Hale; Gh de Monchenault; O. Hamon; J. Kadyak; M. Karolak
The DIRC is a new type of Cherenkov imaging device that will be used for the first time in the BABAR detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long, rectangular bars made from synthetic fused silica as Cherenkov radiator and light guide. The principles of the DIRC ring imaging Cherenkov technique are explained and results from the prototype program are presented. Its choice for the BABAR detector particle identification system is motivated, followed by a discussion of the quartz radiator properties and the detector design.
IEEE Transactions on Nuclear Science | 1998
I. Adam; R. Alcksan; D. Aston; P. Bailly; C. Beigbeder; M. Benayoun; M. Benkebil; G. R. Bonneaud; D. Breton; H. Briand; D. N. Brown; P. Bourgeois; J. Chauveau; R. Cizeron; J. Cohen-Tanugi; M. R. Convery; P. David; C de la Vaissiere; A. de Lesquen; L. Del Buono; G. Fouque; A. Gaidot; F. Gastaldi; J.F. Genat; L. Gosset; Daniel E. Hale; H. Hamel de Monchenault; O. Hamon; J. Kadyk; M. Karolak
The DIRC, a new type of ring-imaging Cherenkov detector that images internally reflected Cherenkov light, is being constructed as the main hadronic particle identification component of the BABAR detector at SLAC. The device makes use of 5 meter long fused silica (colloquially called quartz) bars, which serve both as the Cherenkov radiators and as light pipes for transmitting the light to an array of photo-multiplier tubes. This paper describes a program of research and development aimed at determining whether bars that meet the stringent requirements of the DIRC can be obtained from commercial sources. The results of studies of bulk absorption of fused silica, surface finish, radiation damage and bulk inhomogeneities are discussed.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1993
B. Aubert; A. Bazan; B. Beaugiraud; J. Colas; T. Leflour; M. Maire; J.P. Vialle; I. Wingerter-Seez; Y. Zolnierowski; H. A. Gordon; V. Radeka; D. Rahm; D. Stephani; N. Bulgakov; J.L. Chevalley; C. Fabjan; D. Fournier; O. Gildemeister; P. Jenni; M. Nessi; F. Nessi-Tedaldi; M. Pepe; W. Richter; J. Soderqvist; V. Vuillemin; J.M. Baze; L. Gosset; P. Lavocat; J.P. Lottin; B. Mansoulie
Abstract A prototype of a lead liquid argon accordion calorimeter with two types of cylindrical geometry was constructed and equipped with high speed readout electronics. The energy resolution for electrons is 10%/√E (GeV) with a local constant term of 0.65%. The resolutions obtained for position and angular measurements are given.
nuclear science symposium and medical imaging conference | 1999
I. Adam; R. Aleksan; D. Aston; P. Bailly; C. Beigbeder; M. Benayoun; M. Benkebil; G. R. Bonneaud; D. Breton; H. Briand; D. N. Brown; P. Bourgeois; J. Chauveau; R. Cizeron; J. Cohen-Tanugi; M. R. Convery; S. Dardin; P. David; G. De Domenico; C de la Vaissiere; A. de Lesquen; S. Emery; G. Fouque; A. Gaidot; F. Gastaldi; J.F. Genat; T.L. Geld; L. Gosset; Daniel E. Hale; G. Hamel de Monchenault
The DIRC (acronym for Detection of Internally Reflected Cherenkov (light)) is a new type of Cherenkov ring imaging detector based on total internal reflection that is used for the first time in the BaBar detector at the PEP-II ring of SLAC. The Cherenkov radiators are long rectangular bars made of synthetic fused silica, the photon detector is a water tank equipped with an array of 10,752 conventional photomultipliers. The first year operational experience in the BaBar detector is presented using cosmic data and collision data in the energy region of the /spl Upsi/(4S) resonance.
nuclear science symposium and medical imaging conference | 1991
B. Aubert; A. Bazan; B. Beaugiraud; J. Colas; M. Lebeau; T. Leflour; J.C. MeMarec; M. Maire; P. Petitpas; J. Thion; J.P. Vialle; I. Wingerter-Seez; H. A. Gordon; V. Radeka; D. Rahm; D. Stephani; J.L. Chevalley; C. Fabjan; A. Franz; P. Farthouat; O. Gildemeister; P. Jenni; M. Lefebvre; M. Nessi; F. Nessi-Tedaldi; M. Pepe; W. Richter; G.R. Stevenson; W. Willis; J.M. Baze
Summary form only given. A research and development program is being conducted in view of realizing an electromagnetic and hadronic calorimeter for the Large Hadron Collider (LHC). The authors report on tests on fast electronics, coupled to an electromagnetic prototype calorimeter built with an accordion structure. Three different types of preamplifiers have been used. In two (Si and GaAs hybrids), the preamplifier is operated in liquid argon. In the third one, a common based (Si JFET or GaAs) transistor is in the liquid, the charge preamplifier being outside the cryostat, after about 6 m of 50- Omega cable. The shaping amplifier uses RC-CR filtering. The response to a short current pulse peaks after about 20 ns. When the system is connected to the calorimeter, the liquid argon signals peak, as expected, after 30 ns. Noise, linearity, and cross-talk between channels were investigated. First results from an exposure of the calorimeter to electrons of energy 30 to 175 GeV were obtained.<<ETX>>
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University of Texas Health Science Center at San Antonio
View shared research outputsLaboratoire d'Annecy-le-Vieux de physique des particules
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