"A search for squarks and gluinos in final states containing jets, missing transverse momentum and no electrons or muons is presented. The data were recorded by the ATLAS experiment in root s = 7 TeV proton-proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation was observed in 35 pb(-1) of analysed data. Gluino masses below 500 GeV are excluded at the 95% confidence level in simplified models containing only squarks of the first two generations, a gluino octet and a massless neutralino. The exclusion increases to 870 GeV for equal mass squarks and gluinos. In MSUGRA\/CMSSM models with tan beta = 3, A(0) = 0 and mu > 0, squarks and gluinos of equal mass are excluded below 775 GeV. These are the most stringent limits to date. (C) 2011 CERN. Published by Elsevier B.V. All rights reserved."
Aad, G., Abdallah, J., Abdelalim, A.a., Abdesselam, A., Abdinov, O., Abi, B., et al. (2011). Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in root s=7 TeV proton-proton collisions. PHYSICS LETTERS. SECTION B, 701(2), 186-203 [10.1016/j.physletb.2011.05.061].
Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in root s=7 TeV proton-proton collisions
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Liu M; Liu S; Liu Y; Livan M; Livermore SSA; Lleres A; Lloyd SL; Lobodzinska E; Loch P; Lockman WS; Lockwitz S; Loddenkoetter T; Loebinger FK; Loginov A; Loh CW; Lohse T; Lohwasser K; Lokajicek M; Loken J; Lombardo VP; Long RE; Lopes L; Mateos DL; Losada M; Loscutoff P; Lo Sterzo F; Losty MJ; Lou X; Lounis A; Loureiro KF; Love J; Love PA; Lowe AJ; Lu F; Lu J; Lu L; Lubatti HJ; Luci C; Lucotte A; Ludwig A; Ludwig D; Ludwig I; Ludwig J; Luehring F; Luijckx G; Lumb D; Luminari L; Lund E; Lund Jensen B; Lundberg B; Lundberg J; Lundquist J; Lungwitz M; Lupi A; Lutz G; Lynn D; Lys J; Lytken E; Ma H; Ma LL; Goia IM; Maccarrone G; Macchiolo A; Macek B; Miguens JM; Macina D; Mackeprang R; Madaras RJ; Mader WF; Maenner R; Maeno T; Mattig P; Mattig S; Martins PJM; Magnoni L; Magradze E; Magrath CA; Mahalalel Y; Mahboubi K; Mahout G; Maiani C; Maidantchik C; Maio A; Majewski S; Makida Y; Makovec N; Mal R; Malecki P; Malecki R; Maleev VP; Malek F; Mallik U; Malon D; Maltezos S; Malyshev V; Malyukov S; Mameghani R; Mamuzic J; Manabe A; Mandelli L; Mandic I; Mandrysch R; Maneira J; Mangeard PS; Manjavidze ID; Mann A; Manning PM; Manousakis Katsikakis A; Mansoulie B; Manz A; Mapelli A; Mapelli L; March L; Marchand JF; Marchese F; Marchesotti M; Marchiori G; Marcisovsky M; Marin A; Marino CP; Marroquim F; Marshall R; Marshall Z; Martens FK; Marti Garcia S; Martin AJ; Martin B; Martin B; Martin FF; Martin JP; Martin P; Martin TA; Latour BMD; Martinez M; Outschoorn VM; Martyniuk AC; Marx M; Marzano F; Marzin A; Masetti L; Mashimo T; Mashinistov R; Masik J; Maslennikov AL; Mass M; Massa I; Massaro G; Massol N; Mastroberardino A; Masubuchi T; Mathes M; Matricon P; Matsumoto H; Matsunaga H; Matsushita T; Mattravers C; Maugain JM; Maxfield SJ; Maximov DA; May EN; Mayne A; Mazini R; Mazur M; Mazzanti M; Mazzoni E; McKee SP; McCarn A; McCarthy RL; McCarthy TG; McCubbin NA; McFarlane KW; Mcfayden JA; McGlone H; Mchedlidze G; McLaren RA; Mclaughlan T; McMahon SJ; McPherson RA; Meade A; Mechnich J; 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SALAMANNA, GIUSEPPE ;Salamon A; Saleem M; Salihagic D; Salnikov A; Salt J; Ferrando BMS; Salvatore D; Salvatore F; Salzburger A; Sampsonidis D; Samset BH; Sandaker H; Sander HG; Sanders MP; Sandhoff M; Sandhu P; Sandoval T; Sandstroem R; Sandvoss S; Sankey DPC; Sansoni A; Rios CS; Santoni C; Santonico R; Santos H; Saraiva JG; Sarangi T; Sarkisyan Grinbaum E; Sarri F; Sartisohn G; Sasaki O; Sasaki T; Sasao N; Satsounkevitch I; Sauvage G; Sauvan JB; Savard P; Savinov V; Savu DO; Savva P; Sawyer L; Saxon DH; Says LP; Sbarra C; Sbrizzi A; Scallon O; Scannicchio DA; Schaarschmidt J; Schacht P; Schafer U; Schaetzel S; Schaffer AC; Schaile D; Schamberger RD; Schamov AG; Scharf V; Schegelsky VA; Scheirich D; Scherzer MI; Schiavi C; Schieck J; Schioppa M; Schlenker S; Schlereth JL; Schmidt E; Schmidt MP; Schmieden K; Schmitt C; Schmitz M; Schoning A; Schott M; Schouten D; Schovancova J; Schram M; Schroeder C; Schroer N; Schuh S; Schuler G; Schultes J; Schultz Coulon HC; Schulz H; Schumacher JW; 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Zobernig G; Zoccoli A; Zolnierowski Y; Zsenei A; zur Nedden M; Zutshi V; Zwalinski L.
2011-01-01
Abstract
"A search for squarks and gluinos in final states containing jets, missing transverse momentum and no electrons or muons is presented. The data were recorded by the ATLAS experiment in root s = 7 TeV proton-proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation was observed in 35 pb(-1) of analysed data. Gluino masses below 500 GeV are excluded at the 95% confidence level in simplified models containing only squarks of the first two generations, a gluino octet and a massless neutralino. The exclusion increases to 870 GeV for equal mass squarks and gluinos. In MSUGRA\/CMSSM models with tan beta = 3, A(0) = 0 and mu > 0, squarks and gluinos of equal mass are excluded below 775 GeV. These are the most stringent limits to date. (C) 2011 CERN. Published by Elsevier B.V. All rights reserved."
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.