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    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, Abouzeid Os, H. Abramowicz, H. Abreu, R. Abreu, Y. Abulaiti, Acharya Bs, L. Adamczyk, Adams Dl, J. Adelman, S. Adomeit, T. Adye, T. Agatonovic-Jovin, Aguilar-Saavedra Ja, M. Agustoni, Ahlen Sp, F. Ahmadov, G. Aielli, H. Akerstedt, Åkesson Tpa, G. Akimoto, Akimov Av, Alberghi Gl, J. Albert, S. Albrand, Alconada Verzini Mj, M. Aleksa, Aleksandrov In, C. Alexa, G. Alexander, G. Alexandre, T. Alexopoulos, M. Alhroob, G. Alimonti, L. Alio, Allbrooke Bmm, Allison Lj, Allport Pp, J. Almond, A. Aloisio, A. Alonso, F. Alonso, C. Alpigiani, A. Altheimer, B. Alvarez Gonzalez, Alviggi Mg, K. Amako, Y. Amaral Coutinho, C. Amelung, D. Amidei, Amor Dos Santos Sp, A. Amorim, S. Amoroso, N. Amram, G. Amundsen, C. Anastopoulos, Ancu Ls, N. Andari, T. Andeen, Anders Cf, G. Anders, Anderson Kj, A. Andreazza, V. Andrei, Anduaga Xs, S. Angelidakis, I. Angelozzi, P. Anger, A. Angerami, and Anghinolfi,
    © 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