•  3
    The ATLAS Simulation Infrastructure
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, Abdelalim Aa, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, Bs Acharya, Dl Adams, Tn Addy, J. Adelman, C. Adorisio, P. Adragna, T. Adye, S. Aefsky, Ja Aguilar-Saavedra, M. Aharrouche, Sp Ahlen, F. Ahles, A. Ahmad, H. Ahmed, M. Ahsan, G. Aielli, T. Akdogan, Tpa Åkesson, G. Akimoto, Akimov Av, A. Aktas, Ms Alam, Ma Alam, S. Albrand, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, Alison J., M. Aliyev, Pp Allport, Se Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, Mg Alviggi, K. Amako, C. Amelung, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, Cf Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, S. Antonelli, J. Antos, B. Antunovic, F. Anulli, S. Aoun, G. Arabidze, I. Aracena, Y. Arai, Ath Arce, Jp Archambault, S. Arfaoui, Jf Arguin, T. Argyropoulos, M. Arik, Aj Armbruster, O. Arnaez, C. Arnault, A. Artamonov, and D. Arutinov
    The simulation software for the ATLAS Experiment at the Large Hadron Collider is being used for large-scale production of events on the LHC Computing Grid. This simulation requires many components, from the generators that simulate particle collisions, through packages simulating the response of the various detectors and triggers. All of these components come together under the ATLAS simulation infrastructure. In this paper, that infrastructure is discussed, including that supporting the detecto…Read more
  •  2
    Drift Time Measurement in the ATLAS Liquid Argon Electromagnetic Calorimeter using Cosmic Muons
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, Abdelalim Aa, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, Bs Acharya, Dl Adams, Tn Addy, J. Adelman, C. Adorisio, P. Adragna, T. Adye, S. Aefsky, Ja Aguilar-Saavedra, M. Aharrouche, Sp Ahlen, F. Ahles, A. Ahmad, H. Ahmed, M. Ahsan, G. Aielli, T. Akdogan, Tpa Åkesson, G. Akimoto, Akimov Av, A. Aktas, Ms Alam, Ma Alam, Albert J., S. Albrand, M. Aleksa, In Aleksandrov, F. Alessandria, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, Alison J., M. Aliyev, Pp Allport, Se Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, Mg Alviggi, K. Amako, C. Amelung, Vv Ammosov, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, Cf Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Antonaki, M. Antonelli, S. Antonelli, J. Antos, B. Antunovic, F. Anulli, S. Aoun, G. Arabidze, I. Aracena, Y. Arai, Ath Arce, Jp Archambault, S. Arfaoui, Jf Arguin, T. Argyropoulos, E. Arik, M. Arik, and Aj Armbruster
    The ionization signals in the liquid argon of the ATLAS electromagnetic calorimeter are studied in detail using cosmic muons. In particular, the drift time of the ionization electrons is measured and used to assess the intrinsic uniformity of the calorimeter gaps and estimate its impact on the constant term of the energy resolution. The drift times of electrons in the cells of the second layer of the calorimeter are uniform at the level of 1.3% in the barrel and 2.8% in the endcaps. This leads t…Read more
  •  6
    Readiness of the ATLAS liquid argon calorimeter for LHC collisions
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, Abdelalim Aa, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, Bs Acharya, Dl Adams, Tn Addy, J. Adelman, C. Adorisio, P. Adragna, T. Adye, S. Aefsky, Ja Aguilar-Saavedra, M. Aharrouche, Sp Ahlen, F. Ahles, A. Ahmad, H. Ahmed, M. Ahsan, G. Aielli, T. Akdogan, Tpa Åkesson, G. Akimoto, Akimov Av, A. Aktas, Ms Alam, Ma Alam, Albert J., S. Albrand, M. Aleksa, In Aleksandrov, F. Alessandria, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, Alison J., M. Aliyev, Pp Allport, Se Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, Mg Alviggi, K. Amako, C. Amelung, Vv Ammosov, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, Cf Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Antonaki, M. Antonelli, S. Antonelli, B. Antunovic, F. Anulli, S. Aoun, G. Arabidze, I. Aracena, Y. Arai, Ath Arce, Jp Archambault, S. Arfaoui, Jf Arguin, T. Argyropoulos, E. Arik, and M. Arik
    The ATLAS liquid argon calorimeter has been operating continuously since August 2006. At this time, only part of the calorimeter was readout, but since the beginning of 2008, all calorimeter cells have been connected to the ATLAS readout system in preparation for LHC collisions. This paper gives an overview of the liquid argon calorimeter performance measured in situ with random triggers, calibration data, cosmic muons, and LHC beam splash events. Results on the detector operation, timing perfor…Read more
  •  14
    Commissioning of the ATLAS Muon Spectrometer with cosmic rays
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, Abdelalim Aa, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, Bs Acharya, Dl Adams, Tn Addy, J. Adelman, C. Adorisio, P. Adragna, T. Adye, S. Aefsky, Ja Aguilar-Saavedra, M. Aharrouche, Sp Ahlen, F. Ahles, A. Ahmad, H. Ahmed, M. Ahsan, G. Aielli, T. Akdogan, Tpa Åkesson, G. Akimoto, Akimov Av, A. Aktas, Ms Alam, Ma Alam, S. Albrand, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, Alison J., M. Aliyev, Pp Allport, Se Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, Mg Alviggi, K. Amako, C. Amelung, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, Cf Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, S. Antonelli, J. Antos, B. Antunovic, F. Anulli, S. Aoun, G. Arabidze, I. Aracena, Y. Arai, Ath Arce, Jp Archambault, S. Arfaoui, Jf Arguin, T. Argyropoulos, M. Arik, Aj Armbruster, O. Arnaez, C. Arnault, and A. Artamonov
    The ATLAS detector at the Large Hadron Collider has collected several hundred million cosmic ray events during 2008 and 2009. These data were used to commission the Muon Spectrometer and to study the performance of the trigger and tracking chambers, their alignment, the detector control system, the data acquisition and the analysis programs. We present the performance in the relevant parameters that determine the quality of the muon measurement. We discuss the single element efficiency, resoluti…Read more
  •  2
    The ATLAS Inner Detector commissioning and calibration
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, Abdelalim Aa, A. Abdesselam, O. Abdinov, B. Abi, M. Abolins, H. Abramowicz, H. Abreu, Bs Acharya, Dl Adams, Tn Addy, J. Adelman, C. Adorisio, P. Adragna, T. Adye, S. Aefsky, Ja Aguilar-Saavedra, M. Aharrouche, Sp Ahlen, F. Ahles, A. Ahmad, M. Ahsan, G. Aielli, T. Akdogan, Tpa Åkesson, G. Akimoto, Akimov Av, A. Aktas, Ms Alam, Ma Alam, S. Albrand, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, M. Aliev, G. Alimonti, Alison J., M. Aliyev, Pp Allport, Se Allwood-Spiers, J. Almond, A. Aloisio, R. Alon, A. Alonso, Mg Alviggi, K. Amako, C. Amelung, G. Amorós, N. Amram, C. Anastopoulos, T. Andeen, Cf Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, A. Angerami, F. Anghinolfi, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, S. Antonelli, J. Antos, B. Antunovic, F. Anulli, S. Aoun, G. Arabidze, I. Aracena, Y. Arai, Ath Arce, Jp Archambault, S. Arfaoui, Jf Arguin, T. Argyropoulos, M. Arik, Aj Armbruster, O. Arnaez, C. Arnault, and A. Artamonov
    The ATLAS Inner Detector is a composite tracking system consisting of silicon pixels, silicon strips and straw tubes in a 2 T magnetic field. Its installation was completed in August 2008 and the detector took part in data-taking with single LHC beams and cosmic rays. The initial detector operation, hardware commissioning and in-situ calibrations are described. Tracking performance has been measured with 7. 6 million cosmic-ray events, collected using a tracking trigger and reconstructed with mo…Read more
  •  2
    Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at √s= TeV with the ATLAS detector
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, S. Abdel Khalek, O. Abdinov, R. Aben, B. Abi, M. Abolins, Os Abouzeid, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Bs Acharya, L. Adamczyk, Dl Adams, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Ja Aguilar-Saavedra, M. Agustoni, Sp Ahlen, F. Ahmadov, G. Aielli, H. Akerstedt, Tpa Åkesson, G. Akimoto, Akimov Av, Gl Alberghi, Albert J., S. Albrand, Mj Alconada Verzini, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, Alison J., Bmm Allbrooke, Allison Lj, Pp Allport, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, B. Alvarez Gonzalez, Mg Alviggi, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Sp Amor Dos Santos, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ls Ancu, N. Andari, T. Andeen, Cf Anders, G. Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, A. Antonov, J. Antos, and Anulli
    © 2014, The Author.: A search for the neutral Higgs bosons predicted by the Minimal Supersymmetric Standard Model is reported. The analysis is performed on data from proton-proton collisions at a centre-of-mass energy of 8 TeV collected with the ATLAS detector at the Large Hadron Collider. The samples used for this search were collected in 2012 and correspond to integrated luminosities in the range 19.5-20.3 fb−1. The MSSM Higgs bosons are searched for in the τ τ final state. No significant exce…Read more
  •  2
    Search for pair and single production of new heavy quarks that decay to a Z boson and a third-generation quark in pp collisions at TeV with the ATLAS detector
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, S. Abdel Khalek, O. Abdinov, R. Aben, B. Abi, M. Abolins, Os Abouzeid, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Bs Acharya, L. Adamczyk, Dl Adams, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Ja Aguilar-Saavedra, M. Agustoni, Sp Ahlen, F. Ahmadov, G. Aielli, H. Akerstedt, Tpa Åkesson, G. Akimoto, Akimov Av, Gl Alberghi, Albert J., S. Albrand, Mj Alconada Verzini, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, Alison J., Bmm Allbrooke, Allison Lj, Pp Allport, J. Almond, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, B. Alvarez Gonzalez, Mg Alviggi, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Sp Amor Dos Santos, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ls Ancu, N. Andari, T. Andeen, Cf Anders, G. Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, and A. Antonov
    © 2014, The Author.: A search is presented for the production of new heavy quarks that decay to a Z boson and a third-generation Standard Model quark. In the case of a new charge +2/3 quark, the decay targeted is T → Zt, while the decay targeted for a new charge −1/3 quark is B → Zb. The search is performed with a dataset corresponding to 20.3 fb −1 of pp collisions at TeV recorded in 2012 with the ATLAS detector at the CERN Large Hadron Collider. Selected events contain a high transverse moment…Read more
  •  2
    Measurement of the W W + W Z cross section and limits on anomalous triple gauge couplings using final states with one lepton, missing transverse momentum, and two jets with the ATLAS detector at √s = 7 TeV
    with Atlasc The, G. Aad, B. Abbott, J. Abdallah, S. Abdel Khalek, O. Abdinov, R. Aben, B. Abi, M. Abolins, Os Abouzeid, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Bs Acharya, L. Adamczyk, Dl Adams, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Ja Aguilar-Saavedra, M. Agustoni, Sp Ahlen, F. Ahmadov, G. Aielli, H. Akerstedt, Tpa Åkesson, G. Akimoto, Akimov Av, Gl Alberghi, Albert J., S. Albrand, Mj Alconada Verzini, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, Alison J., Bmm Allbrooke, Allison Lj, Pp Allport, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, B. Alvarez Gonzalez, Mg Alviggi, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Sp Amor Dos Santos, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ls Ancu, N. Andari, T. Andeen, Cf Anders, G. Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, A. Antonov, J. Antos, and Anulli
    © 2015, The Author.: The production of a W boson decaying to eν or μν in association with a W or Z boson decaying to two jets is studied using 4.6 fb−1 of proton-proton collision data at √s =7 TeV recorded with the ATLAS detector at the LHC. The combined WW + WZ cross section is measured with a significance of 3.4σ and is found to be 68±7 ±19 pb, in agreement with the Standard Model expectation of 61.1±2.2 pb. The distribution of the transverse momentum of the dijet system is used to set limits …Read more
  •  1
    Search for contact interactions and large extra dimensions in the dilepton channel using proton–proton collisions at √s=8 TeV with the ATLAS detector
    with C. Atlas, G. Aad, B. Abbott, J. Abdallah, S. Abdel Khalek, O. Abdinov, R. Aben, B. Abi, M. Abolins, Os Abouzeid, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Bs Acharya, L. Adamczyk, Dl Adams, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Ja Aguilar-Saavedra, M. Agustoni, Sp Ahlen, F. Ahmadov, G. Aielli, H. Akerstedt, Tpa Åkesson, G. Akimoto, Akimov Av, Gl Alberghi, Albert J., S. Albrand, Mj Alconada Verzini, M. Aleksa, In Aleksandrov, Alexa C., G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, Alison J., Bmm Allbrooke, Allison Lj, Pp Allport, J. Almond, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, B. Alvarez Gonzalez, Mg Alviggi, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Sp Amor Dos Santos, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ls Ancu, N. Andari, T. Andeen, Cf Anders, G. Anders, Kj Anderson, A. Andreazza, V. Andrei, Xs Anduaga, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, F. Anghinolfi, Anisenkov Av, N. Anjos, A. Annovi, A. Antonaki, M. Antonelli, A. Antonov, and J. Antos
    © 2014, CERN for the benefit of the ATLAS collaboration.A search is conducted for non-resonant new phenomena in dielectron and dimuon final states, originating from either contact interactions or large extra spatial dimensions. The LHC 2012 proton–proton collision dataset recorded by the ATLAS detector is used, corresponding to 20 fb at = 8 TeV. The dilepton invariant mass spectrum is a discriminating variable in both searches, with the contact interaction search additionally utilizing the dilep…Read more