Performance of the ATLAS electromagnetic calorimeter end-cap module 0

B Aubert ,L Di Ciaccio ,I Wingerter-Seez ,P Puzo ,L Poggioli ,J Collot ,G Parrour ,D Lacour ,W Bertoli ,R Zitoun ,G Costa ,M Chalifour ,Johan Lundqvist ,P.y Duval ,S Rajagopalan ,B Merkel ,G Perrot ,J.p Richer ,M.-L Gallin-Martel ,R Lafaye ,F Henry‐Couannier ,D Benchekroun ,F Lanni ,C Benchouk ,J Farrell ,S Negroni ,M Raymond ,H Cunitz ,L Carminati ,M Moynot ,P Pralavorio ,В Ф Казанин ,N Massol ,F Barreiro ,M Citterio ,C De La Taille ,S Saboumazrag ,A Camard ,L Hinz ,J-Y Hostachy ,R Snopkov ,F Hubaut ,S Rodier ,F Chollet ,P Fassnacht ,C Clément ,V Tocut ,D Nicod ,J Schwindling ,J Belorgey ,J Vossebeld ,L Neukermans ,J Egdemir ,J Prast ,F Astesan ,M Rijssenbeek ,P Pétroff ,X Riccadona ,M Delmastro ,J Hoffman ,L Labarga ,B Dinkespiler ,H Ghazlane ,I Stumer ,J Ballansat ,J Dodd ,В М Малышев ,V Vuillemin ,J Mcdonald ,J J Veillet ,I Falleau ,Olivier J F Martin ,Alexei Maslennikov ,A Clark ,G Battistoni ,F Malek ,Angel Abusleme ,N Cartiglia ,L Moneta ,D Imbault ,Mark Pearce ,J Lesueur ,R Bernard ,D Fournier ,M El Kacimi ,A Chekhtman ,L Martin ,A Shousharo ,P Cros ,M A L Leite ,M Mazzanti ,G M Kolachev ,C.p Marin ,E Nagy ,B Hackenburg ,G Guilhem ,M Leltchouk ,C Driouichi ,J Colás ,H Ma ,A Ben Mansour ,E Augé ,A Le Van Suu ,W Bonivento ,Y Jacquier ,S Hassani ,F Rossel ,F Djama ,D Bretón ,J Tóth ,C Bourdarios ,J Ye,Ph Ghez ,K Yip ,D Rousseau ,Г Е Поспелов ,B Belhorma ,D Makowiecki ,J Del Peso ,J Thion ,J Bán ,A Idrissi ,C Girard ,R L Mccarthy ,J Kierstead ,D Lissauer ,J A Parsons ,V Aulchenko ,M Wielers ,W Willis ,M Fanti ,Ph Schwemling ,C Alexa ,B Lund‐Jensen ,S Tisserant ,W Cleland ,P Delebecque ,Alan Gara ,A Belymam ,R Engelmann ,M Hakimi ,B Mansoulié ,B Canton ,D Rahm ,N Dumont-Dayot ,S Rescia ,C Le Maner ,J.m Noppe ,N Seguin-Moreau ,E Monnier ,V Radeka ,David Martín ,S Fichet ,O Le Dortz ,M Seman ,Stefan Rydström ,P Perrodo ,A Jérémie ,K Kordas ,R Stroynowski ,A Talyshev ,J Teiger ,P Pailler ,B Répetti ,A Bazan ,Philippe A Martin ,Yu A Tikhonov ,H Takai ,P Karst ,G Sauvage ,G G Mace ,S Jézéquel ,A Hoummada ,E.m Abouelouafa ,A Mirea ,B Laforge ,B Beaugiraud ,W Seidl ,H Kambara ,P Schilly ,P Barrillon ,J B Hansen ,L Hervás ,J Bremer ,G F Tartarelli ,I Efthymiopoulos ,H Chen,Linda Megner ,T Leflour ,Rajaa Cherkaoui ,J Boniface ,G Garcı́a ,S Simion ,J.l Chevalley ,J F Renardy ,L Serin ,I Nikolic-Audit ,O Gaumer ,Y Zolnierowski ,J.p Taguet ,D Sauvage ,F Orsini ,Y El Mouahhidi ,D Zerwas ,L Mandelli ,A Le Coroller ,A Ferrari ,H Przysiezniak ,F Gianotti ,M Jevaud ,J Ernwein ,H A Gordon ,W Sippach ,C Olivier ,M Gouanère ,J Steffens

doi:10.1016/s0168-9002(03)00344-9

Performance of the ATLAS electromagnetic calorimeter end-cap module 0

B Aubert , L Di Ciaccio + Show 214 more

Open Access

https://doi.org/10.1016/s0168-9002(03)00344-9

Copy DOI

Journal: Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment	Publication Date: Feb 12, 2003
Citations: 29

Affiliation: Laboratoire d’Annecy de Physique des Particules, Institut National de Physique Nucléaire et de Physique des Particules, French National Centre for Scientific Research

#Pseudorapidity Range #ATLAS Electromagnetic Calorimeter + Show 8 more

Abstract
Full-Text PDF
Similar Papers

Abstract

The construction and beam test results of the ATLAS electromagnetic end-cap calorimeter pre-production module 0 are presented. The stochastic term of the energy resolution is between 10% and 12.5% GeV 1/2 over the full pseudorapidity range. Position and angular resolutions are found to be in agreement with simulation. A global constant term of 0.6% is obtained in the pseudorapidity range 2.5< η<3.2 (inner wheel).

Full Text