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IRIS
Charged-particle fragmentation functions for jets azimuthally balanced by a high-transverse-momentum, prompt, isolated photon are measured in 25 pb(-1) of pp and 0.49 nb(-1) of Pb + Pb collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The measurements are compared to predictions of Monte Carlo generators and to measurements of inclusively selected jets. In pp collisions, a different jet fragmentation function in photon-tagged events from that in inclusive jet events arises from the difference in fragmentation between light quarks and gluons. The ratios of the fragmentation functions in Pb + Pb events to that in pp events are used to explore the parton color-charge dependence of jet quenching in the hot medium. In relatively peripheral collisions, fragmentation functions exhibit a similar modification pattern for photon-tagged and inclusive jets. However, photon-tagged jets are observed to have larger modifications than inclusive jets in central Pb + Pb events.
Aaboud, M., Aad, G., Abbott, B., Abdinov, O., Abeloos, B., Abhayasinghe, D. ., et al. (2019). Comparison of Fragmentation Functions for Jets Dominated by Light Quarks and Gluons from
pp
and
Pb+Pb
Collisions in ATLAS. PHYSICAL REVIEW LETTERS, 123(4) [10.1103/PhysRevLett.123.042001].
Comparison of Fragmentation Functions for Jets Dominated by Light Quarks and Gluons from
pp
and
Pb+Pb
Collisions in ATLAS
Aaboud, M.;Aad, G.;Abbott, B.;Abdinov, O.;Abeloos, B.;Abhayasinghe, D. K.;Abidi, S. H.;AbouZeid, O. S.;Abraham, N. L.;Abramowicz, H.;Abreu, H.;Abulaiti, Y.;Acharya, B. S.;Adachi, S.;Adamczyk, L.;Adelman, J.;Adersberger, M.;Adiguzel, A.;Adye, T.;Affolder, A. A.;Afik, Y.;Agheorghiesei, C.;Aguilar-Saavedra, J. A.;Ahmadov, F.;Aielli, G.;Akatsuka, S.;Åkesson, T. P. A.;Akilli, E.;Akimov, A. V.;Alberghi, G. L.;Albert, J.;Albicocco, P.;Alconada Verzini, M. J.;Alderweireldt, S.;Aleksa, M.;Aleksandrov, I. N.;Alexa, C.;Alexopoulos, T.;Alhroob, M.;Ali, B.;Alimonti, G.;Alison, J.;Alkire, S. P.;Allaire, C.;Allbrooke, B. M. M.;Allen, B. W.;Allport, P. P.;Aloisio, A.;Alonso, A.;Alonso, F.;Alpigiani, C.;Alshehri, A. A.;Alstaty, M. I.;Alvarez Gonzalez, B.;Álvarez Piqueras, D.;Alviggi, M. G.;Amadio, B. T.;Amaral Coutinho, Y.;Ambroz, L.;Amelung, C.;Amidei, D.;Amor Dos Santos, S. P.;Amoroso, S.;Amrouche, C. S.;Anastopoulos, C.;Ancu, L. S.;Andari, N.;Andeen, T.;Anders, C. F.;Anders, J. K.;Anderson, K. 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B.;Nicolaidou, R.;Nielsen, J.;Nikiforou, N.;Nikolaenko, V.;Nikolic-Audit, I.;Nikolopoulos, K.;Nilsson, P.;Ninomiya, Y.;Nisati, A.;Nishu, N.;Nisius, R.;Nitsche, I.;Nitta, T.;Nobe, T.;Noguchi, Y.;Nomachi, M.;Nomidis, I.;Nomura, M. A.;Nooney, T.;Nordberg, M.;Norjoharuddeen, N.;Novak, T.;Novgorodova, O.;Novotny, R.;Nozka, L.;Ntekas, K.;Nurse, E.;Nuti, F.;Oakham, F. G.;Oberlack, H.;Obermann, T.;Ocariz, J.;Ochi, A.;Ochoa, I.;Ochoa-Ricoux, J. P.;O’Connor, K.;Oda, S.;Odaka, S.;Oerdek, S.;Oh, A.;Oh, S. H.;Ohm, C. C.;Oide, H.;Ojeda, M. L.;Okawa, H.;Okazaki, Y.;Okumura, Y.;Okuyama, T.;Olariu, A.;Oleiro Seabra, L. F.;Olivares Pino, S. A.;Oliveira Damazio, D.;Oliver, J. L.;Olsson, M. J. R.;Olszewski, A.;Olszowska, J.;O’Neil, D. C.;Onofre, A.;Onogi, K.;Onyisi, P. U. E.;Oppen, H.;Oreglia, M. J.;Oren, Y.;Orestano, D.;Orlando, N.;O’Rourke, A. A.;Orr, R. S.;Osculati, B.;O’Shea, V.;Ospanov, R.;Otero y Garzon, G.;Otono, H.;Ouchrif, M.;Ould-Saada, F.;Ouraou, A.;Ouyang, Q.;Owen, M.;Owen, R. E.;Ozcan, V. E.;Ozturk, N.;Pacalt, J.;Pacey, H. A.;Pachal, K.;Pacheco Pages, A.;Pacheco Rodriguez, L.;Padilla Aranda, C.;Pagan Griso, S.;Paganini, M.;Palacino, G.;Palazzo, S.;Palestini, S.;Palka, M.;Pallin, D.;Panagoulias, I.;Pandini, C. E.;Panduro Vazquez, J. G.;Pani, P.;Panizzo, G.;Paolozzi, L.;Papadopoulou, T. D.;Papageorgiou, K.;Paramonov, A.;Paredes Hernandez, D.;Paredes Saenz, S. R.;Parida, B.;Parker, A. J.;Parker, K. A.;Parker, M. A.;Parodi, F.;Parsons, J. A.;Parzefall, U.;Pascuzzi, V. R.;Pasner, J. M. P.;Pasqualucci, E.;Passaggio, S.;Pastore, F.;Pasuwan, P.;Pataraia, S.;Pater, J. R.;Pathak, A.;Pauly, T.;Pearson, B.;Pedersen, M.;Pedraza Diaz, L.;Pedro, R.;Peleganchuk, S. V.;Penc, O.;Peng, C.;Peng, H.;Peralva, B. S.;Perego, M. M.;Pereira Peixoto, A. P.;Perepelitsa, D. V.;Peri, F.;Perini, L.;Pernegger, H.;Perrella, S.;Peshekhonov, V. D.;Peters, K.;Peters, R. F. Y.;Petersen, B. A.;Petersen, T. C.;Petit, E.;Petridis, A.;Petridou, C.;Petroff, P.;Petrov, M.;Petrucci, F.;Pettee, M.;Pettersson, N. 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2019-01-01
Abstract
Charged-particle fragmentation functions for jets azimuthally balanced by a high-transverse-momentum, prompt, isolated photon are measured in 25 pb(-1) of pp and 0.49 nb(-1) of Pb + Pb collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The measurements are compared to predictions of Monte Carlo generators and to measurements of inclusively selected jets. In pp collisions, a different jet fragmentation function in photon-tagged events from that in inclusive jet events arises from the difference in fragmentation between light quarks and gluons. The ratios of the fragmentation functions in Pb + Pb events to that in pp events are used to explore the parton color-charge dependence of jet quenching in the hot medium. In relatively peripheral collisions, fragmentation functions exhibit a similar modification pattern for photon-tagged and inclusive jets. However, photon-tagged jets are observed to have larger modifications than inclusive jets in central Pb + Pb events.
Aaboud, M., Aad, G., Abbott, B., Abdinov, O., Abeloos, B., Abhayasinghe, D. ., et al. (2019). Comparison of Fragmentation Functions for Jets Dominated by Light Quarks and Gluons from
pp
and
Pb+Pb
Collisions in ATLAS. PHYSICAL REVIEW LETTERS, 123(4) [10.1103/PhysRevLett.123.042001].
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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.
