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Benvenuti nell'Anagrafe della Ricerca d'Ateneo
The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS detector using proton–proton collision data with a centre-of-mass energy of s√=7 TeV corresponding to an integrated luminosity of 4.7 fb −1 . Jets are reconstructed from energy deposits forming topological clusters of calorimeter cells using the anti- kt algorithm with distance parameters R=0.4 or R=0.6 , and are calibrated using MC simulations. A residual JES correction is applied to account for differences between data and MC simulations. This correction and its systematic uncertainty are estimated using a combination of in situ techniques exploiting the transverse momentum balance between a jet and a reference object such as a photon or a Z boson, for 20≤pjetT<1000 GeV and pseudorapidities |η|<4.5 . The effect of multiple proton–proton interactions is corrected for, and an uncertainty is evaluated using in situ techniques. The smallest JES uncertainty of less than 1 % is found in the central calorimeter region ( |η|<1.2 ) for jets with 55≤pjetT<500 GeV . For central jets at lower pT , the uncertainty is about 3 %. A consistent JES estimate is found using measurements of the calorimeter response of single hadrons in proton–proton collisions and test-beam data, which also provide the estimate for pjetT>1 TeV. The calibration of forward jets is derived from dijet pT balance measurements. The resulting uncertainty reaches its largest value of 6 % for low- pT jets at |η|=4.5 . Additional JES uncertainties due to specific event topologies, such as close-by jets or selections of event samples with an enhanced content of jets originating from light quarks or gluons, are also discussed. The magnitude of these uncertainties depends on the event sample used in a given physics analysis, but typically amounts to 0.5–3 %.
Aad, G., Abajyan, T., Abbott, B., Abdallah, J., Abdel Khalek, S., Abdinov, O., et al. (2015). Jet energy measurement and its systematic uncertainty in proton-proton collisions at root s=7 TeV with the ATLAS detector. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS, 75(1), 1-101 [10.1140/epjc/s10052-014-3190-y].
Jet energy measurement and its systematic uncertainty in proton-proton collisions at root s=7 TeV with the ATLAS detector
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Masetti;T. Mashimo;R. Mashinistov;J. Masik;A. L. Maslennikov;I. Massa;N. Massol;P. Mastrandrea;A. Mastroberardino;T. Masubuchi;H. Matsunaga;T. Matsushita;P. Mättig;S. Mättig;J. Mattmann;C. Mattravers;J. Maurer;S. J. Maxfield;D. A. Maximov;R. Mazini;L. Mazzaferro;M. Mazzanti;G. Mc Goldrick;S. P. Mc Kee;A. McCarn;R. L. McCarthy;T. G. McCarthy;N. A. McCubbin;K. W. McFarlane;J. A. Mcfayden;G. Mchedlidze;T. Mclaughlan;S. J. McMahon;R. A. McPherson;A. Meade;J. Mechnich;M. Mechtel;M. Medinnis;S. Meehan;R. Meera-Lebbai;S. Mehlhase;A. Mehta;K. Meier;C. Meineck;B. Meirose;C. Melachrinos;B. R. Mellado Garcia;F. Meloni;L. Mendoza Navas;A. Mengarelli;S. Menke;E. Meoni;K. M. Mercurio;S. Mergelmeyer;N. Meric;P. Mermod;L. Merola;C. Meroni;F. S. Merritt;H. Merritt;A. Messina;J. Metcalfe;A. S. Mete;C. Meyer;C. Meyer;J-P. Meyer;J. Meyer;J. Meyer;S. Michal;R. P. Middleton;S. Migas;L. Mijović;G. Mikenberg;M. Mikestikova;M. Mikuž;D. W. Miller;C. Mills;A. Milov;D. A. Milstead;D. Milstein;A. A. Minaenko;M. 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Prokoshin;E. Protopapadaki;S. Protopopescu;J. Proudfoot;X. Prudent;M. Przybycien;H. Przysiezniak;S. Psoroulas;E. Ptacek;E. Pueschel;D. Puldon;M. Purohit;P. Puzo;Y. Pylypchenko;J. Qian;A. Quadt;D. R. Quarrie;W. B. Quayle;D. Quilty;V. Radeka;V. Radescu;S. K. Radhakrishnan;P. Radloff;F. Ragusa;G. Rahal;S. Rajagopalan;M. Rammensee;M. Rammes;A. S. Randle-Conde;C. Rangel-Smith;K. Rao;F. Rauscher;T. C. Rave;T. Ravenscroft;M. Raymond;A. L. Read;D. M. Rebuzzi;A. Redelbach;G. Redlinger;R. Reece;K. Reeves;A. Reinsch;H. Reisin;I. Reisinger;M. Relich;C. Rembser;Z. L. Ren;A. Renaud;M. Rescigno;S. Resconi;B. Resende;P. Reznicek;R. Rezvani;R. Richter;M. Ridel;P. Rieck;M. Rijssenbeek;A. Rimoldi;L. Rinaldi;E. Ritsch;I. Riu;G. Rivoltella;F. Rizatdinova;E. Rizvi;S. H. Robertson;A. Robichaud-Veronneau;D. Robinson;J. E. M. Robinson;A. Robson;J. G. Rocha de Lima;C. Roda;D. Roda Dos Santos;L. Rodrigues;S. Roe;O. Røhne;S. Rolli;A. Romaniouk;M. Romano;G. Romeo;E. Romero Adam;N. Rompotis;L. Roos;E. Ros;S. Rosati;K. Rosbach;A. Rose;M. Rose;P. L. Rosendahl;O. Rosenthal;V. Rossetti;E. Rossi;L. P. Rossi;R. Rosten;M. Rotaru;I. Roth;J. Rothberg;D. Rousseau;C. R. Royon;A. Rozanov;Y. Rozen;X. Ruan;F. Rubbo;I. Rubinskiy;V. I. Rud;C. Rudolph;M. S. Rudolph;F. Rühr;A. Ruiz-Martinez;L. Rumyantsev;Z. Rurikova;N. A. Rusakovich;A. Ruschke;J. P. Rutherfoord;N. Ruthmann;P. Ruzicka;Y. F. Ryabov;M. Rybar;G. Rybkin;N. C. Ryder;A. F. Saavedra;S. Sacerdoti;A. Saddique;I. Sadeh;H. F-W. Sadrozinski;R. Sadykov;F. Safai Tehrani;H. Sakamoto;Y. Sakurai;G. Salamanna;A. Salamon;M. Saleem;D. Salek;P. H. Sales De Bruin;D. Salihagic;A. Salnikov;J. Salt;B. M. Salvachua Ferrando;D. Salvatore;F. Salvatore;A. Salvucci;A. Salzburger;D. Sampsonidis;A. Sanchez;J. Sánchez;V. Sanchez Martinez;H. Sandaker;H. G. Sander;M. P. Sanders;M. Sandhoff;T. Sandoval;C. Sandoval;R. Sandstroem;D. P. C. Sankey;A. Sansoni;C. Santoni;R. Santonico;H. Santos;I. Santoyo Castillo;K. Sapp;A. Sapronov;J. G. Saraiva;E. Sarkisyan-Grinbaum;B. 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Zaytsev;C. Zeitnitz;M. Zeman;A. Zemla;K. Zengel;O. Zenin;T. Ženiš;D. Zerwas;G. Zevi della Porta;D. Zhang;H. Zhang;J. Zhang;L. Zhang;X. Zhang;Z. Zhang;Z. Zhao;A. Zhemchugov;J. Zhong;B. Zhou;L. Zhou;N. Zhou;C. G. Zhu;H. Zhu;J. Zhu;Y. Zhu;X. Zhuang;A. Zibell;D. Zieminska;N. I. Zimine;C. Zimmermann;R. Zimmermann;S. Zimmermann;S. Zimmermann;Z. Zinonos;M. Ziolkowski;R. Zitoun;G. Zobernig;A. Zoccoli;M. zur Nedden;G. Zurzolo;V. Zutshi;L. Zwalinski
2015-01-01
Abstract
The jet energy scale (JES) and its systematic uncertainty are determined for jets measured with the ATLAS detector using proton–proton collision data with a centre-of-mass energy of s√=7 TeV corresponding to an integrated luminosity of 4.7 fb −1 . Jets are reconstructed from energy deposits forming topological clusters of calorimeter cells using the anti- kt algorithm with distance parameters R=0.4 or R=0.6 , and are calibrated using MC simulations. A residual JES correction is applied to account for differences between data and MC simulations. This correction and its systematic uncertainty are estimated using a combination of in situ techniques exploiting the transverse momentum balance between a jet and a reference object such as a photon or a Z boson, for 20≤pjetT<1000 GeV and pseudorapidities |η|<4.5 . The effect of multiple proton–proton interactions is corrected for, and an uncertainty is evaluated using in situ techniques. The smallest JES uncertainty of less than 1 % is found in the central calorimeter region ( |η|<1.2 ) for jets with 55≤pjetT<500 GeV . For central jets at lower pT , the uncertainty is about 3 %. A consistent JES estimate is found using measurements of the calorimeter response of single hadrons in proton–proton collisions and test-beam data, which also provide the estimate for pjetT>1 TeV. The calibration of forward jets is derived from dijet pT balance measurements. The resulting uncertainty reaches its largest value of 6 % for low- pT jets at |η|=4.5 . Additional JES uncertainties due to specific event topologies, such as close-by jets or selections of event samples with an enhanced content of jets originating from light quarks or gluons, are also discussed. The magnitude of these uncertainties depends on the event sample used in a given physics analysis, but typically amounts to 0.5–3 %.
Aad, G., Abajyan, T., Abbott, B., Abdallah, J., Abdel Khalek, S., Abdinov, O., et al. (2015). Jet energy measurement and its systematic uncertainty in proton-proton collisions at root s=7 TeV with the ATLAS detector. THE EUROPEAN PHYSICAL JOURNAL. C, PARTICLES AND FIELDS, 75(1), 1-101 [10.1140/epjc/s10052-014-3190-y].
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11590/119562
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simulazione ASN
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.