Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using (Formula presented.) TeV proton-proton collision data

P Jackson,N Soni,MJ White,J Bouffard,W Edson,J Ernst, A Fischer,S Guindon, Jain, AI Butt, P Czodrowski,DM Gingrich, RW Moore, JL Pinfold, A Saddique, A Sbrizzi,HS Subramania, FV Vaque, O Cakir,AK Ciftci,R Ciftci,HD Yildiz,S Kuday, M Yilmaz,S Sultansoy, IT Cakir,Z Barnovska, N Berger, M Delmastro,L Di Ciaccio,Tko Doan,S Elles, C Goy,T Hryn ova, S Jézéquel, H Keoshkerian,I Koletsou,R Lafaye, J Levêque, VP Lombardo, N Massol, H Przysiezniak, G Sauvage, E Sauvan, M Schwoerer, O Simard, T Todorov, I Wingerter-Seez, L Asquith, B Auerbach, RE Blair, S Chekanov,JT Childers, EJ Feng,AT Goshaw, T LeCompte, J Love,D Malon, DH Nguyen, L Nodulman, A Paramonov, LE Price, J Proudfoot, Bms Ferrando, RW Stanek,P van Gemmeren,A Vaniachine,R Yoshida,J Zhang,E Cheu, KA Johns, Kaushik, CL Lampen, W Lampl,X Lei, R Leone, P Loch, R Nayyar, F O grady, JP Rutherfoord, MA Shupe, B Toggerson,EW Varnes, J Veatch,A Brandt, D Côté,S Darmora, K De,A Farbin,J Griffiths,HK Hadavand, L Heelan,HY Kim, M Maeno, P 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Buanes, O Dale, G Eigen, A Kastanas, W Liebig,A Lipniacka, BM dit Latour, PL Rosendahl, H Sandaker, TB Sjursen, L Smestad, B Stugu, M Ugland, RM Barnett,J Beringer, J Biesiada,G Brandt, J Brosamer, P Calafiura,LM Caminada, F Cerutti, A Ciocio, RN Clarke, M Cooke, K Copic, S Dube, K Einsweiler,M Garcia-Sciveres, M Gilchriese, C Haber, M Hance, B Heinemann, I Hinchliffe, TR Holmes, M Hurwitz, L Jeanty, W Lavrijsen, C Leggett, P Loscutoff, Z Marshall, A Ovcharova,SP Griso,K Potamianos, A Pranko, Quarrie,M Shapiro, A Sood, MJ Tibbetts, Tsulaia, J Virzi, H Wang,W-M Yao,Yu,EB Kuutmann, FM Giorgi,S Grancagnolo, GH Herbert, R Herrberg-Schubert, I Hristova, O Kind, H Kolanoski, H Lacker, T Lohse, A Nikiforov, L Rehnisch, P Rieck, H Schulz,D Wendland,M zur Nedden, M Agustoni, HP Beck, A Cervelli, A Ereditato, Gallo, S Haug, T Kruker, LF Marti, F Meloni,B Schneider, FG Sciacca, ME Stramaglia, SA Stucci, Weber,Bmm Allbrooke,LA Bella, HS Bansil, J Bracinik, DG Charlton,AS Chisholm,AC Daniells, CM 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Sarrazin, S Schaepe, MJ Schultens, T Schwindt, F Scutti,JA Stillings,N Tannoury, J Therhaag, K Uchida, M Uhlenbrock,A Vogel,E von Toerne, P Wagner, T Wang, N Wermes, P Wienemann, Lam Wiik-Fuchs, BT Winter, Khy Wong, R Zimmermann, S Zimmermann, SP Ahlen, C Bernard, KM Black, JM Butler, L Dell Asta, L Helary, M Kruskal, Ba Long, JT Shank,Z Yan,S Youssef, C Amelung, G Amundsen, G Artoni, Bensinger,L Bianchini,C Blocker,L Coffey, EA Fitzgerald, S Gozpinar, G Sciolla, A Venturini, S Zambito,K Zengel,YA Coutinho, LP Caloba, C Maidantchik, F Marroquim, AA Nepomuceno, JM Seixas, AS Cerqueira, LM de Andrade Filho, Mab do Vale, M Donadelli, Mal Leite, DL Adams,K Assamagan,M Begel,H Chen,Chernyatin,R Debbe, M Ernst, B Gibbard,HA Gordon,X Hu,A Klimentov, A Kravchenko, F Lanni, D Lissauer, D Lynn, H Ma, T Maeno, J Metcalfe, E Mountricha, P Nevski,H Okawa,DO Damazio, F Paige,S Panitkin, DV Perepelitsa, M-A Pleier, Polychronakos, S Protopopescu, M Purohit, Radeka, S Rajagopalan, G Redlinger, J Schovancova, S Snyder, P Steinberg,H Takai, N Triplett, A Undrus, T Wenaus, S Ye,C Alexa, E Badescu,Boldea,SI Buda,I Caprini,M Caprini, A Chitan, M Ciubancan, S Constantinescu, C-M Cuciuc, P Dita, S Dita, OA Ducu, A Jinaru,J Maurer,A Olariu, D Pantea, M Rotaru,G Stoicea, A Tudorache, Tudorache,GA Popeneciu,G Otero y Garzon, R Piegaia, H Reisin, S Sacerdoti, M Arratia, N Barlow, Batley, FM Brochu, W Buttinger,Carter,JD Chapman,G Cottin, ST French, JA Frost, Tps Gillam, JC Hill, S Kaneti, TJ Khoo, CG Lester,T Mueller,MA Parker,D Robinson, T Sandoval

user-5f1f7d444c775e3a796188dc(2014)

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摘要
Abstract: A search for squarks and gluinos in final states containing high-p jets, missing transverse momentum and no electrons or muons is presented. The data were recorded in 2012 by the ATLAS experiment in (Formula presented.) TeV proton-proton collisions at the Large Hadron Collider, with a total integrated luminosity of 20.3 fb. Results are interpreted in a variety of simplified and specific supersymmetry-breaking models assuming that R-parity is conserved and that the lightest neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 1330 GeV for a simplified model incorporating only a gluino and the lightest neutralino. For a simplified model involving the strong production of first- and second-generation squarks, squark masses below 850 GeV (440 GeV) are excluded for a massless lightest neutralino, assuming mass degenerate (single light-flavour) squarks. In mSUGRA/CMSSM models with tan β = 30, A = −2m and μ > 0, squarks and gluinos of equal mass are excluded for masses below 1700 GeV. Additional limits are set for non-universal Higgs mass models with gaugino mediation and for simplified models involving the pair production of gluinos, each decaying to a top squark and a top quark, with the top squark decaying to a charm quark and a neutralino. These limits extend the region of supersymmetric parameter space excluded by previous searches with the ATLAS detector.[Figure not available: see fulltext.].
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Gluino,Lightest Supersymmetric Particle,Stop squark,Neutralino,Top quark,Gaugino,Higgs boson,Large Hadron Collider,Particle physics,Nuclear physics,Physics
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