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Largest layer of SCT barrel detector

The largest radius layer of the SCT barrel detector after all SCT modules had been mounted in a clean room in the physics department.

Professor Tony Weidberg

Professor of Physics

Research theme

  • Fundamental particles and interactions

Sub department

  • Particle Physics

Research groups

  • ATLAS
Tony.Weidberg@physics.ox.ac.uk
Telephone: 01865 (2)73370
Denys Wilkinson Building, room 629
  • About
  • Publications

Electronics and readout of a large area silicon detector for LHC

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment Elsevier 344:1 (1994) 185-193

Authors:

K Borer, DJ Munday, MA Parker, F Anghinolfi, P Aspell, M Campbell, A Chilingarov, P Jarron, EHM Heijne, JC Santiard, P Scampoli, H Verweij, C Gössling, B Lisowski, A Reichold, R Spiwoks, E Tsesmelis, K Benslama, R Bonino, AG Clark, C Couyoumtzelis, H Kambara, X Wu, E Fretwurst, G Lindstroem, T Schultz, RA Bardos, GW Gorfine, GF Moorhead, GN Taylor, SN Tovey, JH Bibby, RJ Hawkings, N Kundu, A Weidberg, D Campbell, P Murray, P Seller, J Teiger
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APC3-A Charge Sampling, Storage & Readout Chip for Silicon Detector Readout RD2 Collaboration

IEEE Transactions on Nuclear Science 41:4 (1994) 1091-1094

Authors:

K Borer, DJ Munday, MA Parker, F Anghinolfi, P Aspell, M Campbell, P Jarron, EHM Heijne, JC Santiard, H Verweij, C Gößling, A Reichold, R Bonino, AG Clark, H Kambara, DL Marra, A Leger, JP Richeaux, X Wu, F Fares, J Bibby, A Weidberg, D Campbell, P Murray, P Seller, M Rouget, J Teiger

Abstract:

The “APC3” is a charge sampling and storage chip designed for high speed readout of silicon detectors. It has 32 channels, each with preamplifier, integrator and storage capacitors. Current from a silicon detector connected to the input is integrated as a charge and stored on a capacitor. There are 128 capacitors per channel which are used sequentially to store the charge. The charge is held on the storage capacitor until it is either read out or discarded. Logic on the chip manages the storage and retrieval of samples. This logic uses a novel architecture based on a system of pointers and read out addresses. This paper describes the operation of the chip and measurements of its performance. © 1994 IEEE
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Study of neutron irradiated silicon counters with a fast amplifier

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment Elsevier 337:1 (1993) 57-65

Authors:

S Bates, DJ Munday, MA Parker, F Anghinolfi, A Chilingarov, A Ciasnohova, M Glaser, P Jarron, F Lemeilleur, JC Santiard, C Gößling, B Lisowski, S Pilath, A Rolf, R Bonino, AG Clark, H Kambara, X Wu, E Fretwurst, G Lindström, T Schulz, GF Moorhead, GN Taylor, SN Tovey, R Hawkings, A Weidberg, J Teiger
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A study of a second level track trigger for ATLAS

Nuclear Inst. and Methods in Physics Research, A 336:1-2 (1993) 59-77

Authors:

K Borer, S Bates, DJ Munday, MA Parker, A Poppleton, C Gössling, B Lisowski, A Reichold, R Spiwoks, E Tsesmelis, AG Clark, R Bonino, X Wu, GF Moorhead, GN Taylor, SN Tovey, S Stapnes, RJ Hawkings, AR Weidberg, P Lubrano, P Scampoli, J Teiger, A Gheorghe, R Bock, W Krischer

Abstract:

This paper discusses some of the problems of triggering at a high energy, high luminosity pp collider. A suggested second level track trigger for the ATLAS detector is described, based on hit information from a silicon tracker. Detailed Monte Carlo simulations have been performed to assess the performance of the trigger in accepting electrons and in rejecting the QCD jets that would fake electrons in the first level calorimeter trigger. Studies of the feasibility of implementing such a trigger are also presented. © 1993.
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A search for new intermediate vector bosons and excited quarks decaying to two-jets at the CERN p̄p collider

Nuclear Physics, Section B 400:1-3 (1993) 3-22

Authors:

J Alitti, G Ambrosini, R Ansari, D Autiero, P Bareyre, IA Bertram, G Blaylock, P Bonamy, K Borer, M Bourliaud, D Buskulic, G Carboni, D Cavalli, V Cavasinni, P Cenci, JC Chollet, C Conta, G Costa, F Costantini, L Cozzi, A Cravero, M Curatolo, A Dell'Acqua, T DelPrete, RS DeWolf, L DiLella, Y Ducros, GF Egan, KF Einsweiler, B Esposito, L Fayard, A Federspiel, R Ferrari, M Fraternali, D Froidevaux, G Fumagalli, JM Gaillard, F Gianotti, O Gildemeister, C Gössling, VG Goggi, S Grünendahl, K Hara, S Hellman, J Hřivnáč, H Hufnagel, E Hugentobler, K Hultqvist, E Iacopini, J Incandela, K Jakobs, P Jenni, EE Kluge, N Kurz, S Lami, P Lariccia, M Lefebvre, L Linssen, M Livan, P Lubrano, C Magneville, L Malgeri, L Mandelli, L Mapelli, M Mazzanti, K Meier, B Merkel, JP Meyer, M Moniez, R Moning, M Morganti, L Müller, DJ Munday, M Nessi, F Nessi-Tedaldi, C Onions, T Pal, MA Parker, G Parrour, F Pastore, E Pennacchio, JM Pentney, M Pepe, L Perini, C Petridou, P Petroff, H Plothow-Besch, G Polesello, A Poppleton, K Pretzl, M Primavera, M Punturo, JP Repellin, A Rimoldi, M Sacchi, P Scampoli, J Schacher, B Schmidt, V Šimák, SL Singh

Abstract:

The two-jet invariant mass spectrum as measured in the UA2 experiment is used to search for additional heavy vector bosons decaying to two-jets. The mass of an additional W boson that couples to fermions with a V+A form is constrained to be greater than 261 GeV to the 90% confidence level. A limit on the production cross section of additional W and Z bosons is given as a function of the boson mass. A limit on the production of excited quarks is also given as a function of the excited quark mass. © 1993.
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