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IRIS
A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of root s = 13 TeV corresponding to an integrated luminosity of 36.1 fb(-1). Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing b-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical Z' bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross sections, the Z' boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1-3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 to 0.9 TeV and from 2.0 to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.
Aaboud, M., Aad, G., Abbott, B., Abbott, D. ., Abdinov, O., Abeloos, B., et al. (2019). Search for heavy particles decaying into a top-quark pair in the fully hadronic final state in
pp
collisions at
s=13 TeV
with the ATLAS detector. PHYSICAL REVIEW D, 99(9) [10.1103/PhysRevD.99.092004].
Search for heavy particles decaying into a top-quark pair in the fully hadronic final state in
pp
collisions at
s=13 TeV
with the ATLAS detector
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F.;Dang, N. P.;Dann, N. D;Danninger, M.;Dao, V.;Darbo, G.;Darmora, S.;Dartsi, O.;Dattagupta, A.;Daubney, T.;D’Auria, S.;Davey, W.;David, C.;Davidek, T.;Davis, D. R.;Dawe, E.;Dawson, I.;De, K.;De Asmundis, R.;De Benedetti, A.;De Beurs, M.;De Castro, S.;De Cecco, S.;De Groot, N.;de Jong, P.;De la Torre, H.;De Lorenzi, F.;De Maria, A.;De Pedis, D.;De Salvo, A.;De Sanctis, U.;De Santis, M.;De Santo, A.;De Vasconcelos Corga, K.;De Vivie De Regie, J. B.;Debenedetti, C.;Dedovich, D. V.;Dehghanian, N.;Del Gaudio, M.;Del Peso, J.;Delabat Diaz, Y.;Delgove, D.;Deliot, F.;Delitzsch, C. M.;Della Pietra, M.;Della Volpe, D.;Dell’Acqua, A.;Dell’Asta, L.;Delmastro, M.;Delporte, C.;Delsart, P. A.;DeMarco, D. A.;Demers, S.;Demichev, M.;Denisov, S. P.;Denysiuk, D.;D’Eramo, L.;Derendarz, D.;Derkaoui, J. E.;Derue, F.;Dervan, P.;Desch, K.;Deterre, C.;Dette, K.;Devesa, M. R.;Deviveiros, P. O.;Dewhurst, A.;Dhaliwal, S.;Di Bello, F. A.;Di Ciaccio, A.;Di Ciaccio, L.;Di Clemente, W. 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J.;McNamara, P. C.;McNicol, C. J.;McPherson, R. A.;Mdhluli, J. E.;Meadows, Z. A.;Meehan, S.;Megy, T. M.;Mehlhase, S.;Mehta, A.;Meideck, T.;Meirose, B.;Melini, D.;Mellado Garcia, B. R.;Mellenthin, J. D.;Melo, M.;Meloni, F.;Melzer, A.;Menary, S. B.;Mendes Gouveia, E. D.;Meng, L.;Meng, X. T.;Menke, S.;Meoni, E.;Mergelmeyer, S.;Merkt, S. A. M.;Merlassino, C.;Mermod, P.;Merola, L.;Meroni, C.;Merritt, F. S.;Messina, A.;Metcalfe, J.;Mete, A. S.;Meyer, C.;Meyer, J.;Meyer, J-P.;Meyer Zu Theenhausen, H.;Miano, F.;Middleton, R. P.;Mijović, L.;Mikenberg, G.;Mikestikova, M.;Mikuž, M.;Milesi, M.;Milic, A.;Millar, D. A.;Miller, D. W.;Milov, A.;Milstead, D. A.;Mina, R. A.;Minaenko, A. A.;Miñano Moya, M.;Minashvili, I. A.;Mincer, A. I.;Mindur, B.;Mineev, M.;Minegishi, Y.;Ming, Y.;Mir, L. M.;Mirto, A.;Mistry, K. P.;Mitani, T.;Mitrevski, J.;Mitsou, V. A.;Mittal, M.;Miucci, A.;Miyagawa, P. S.;Mizukami, A.;Mjörnmark, J. U.;Mkrtchyan, T.;Mlynarikova, M.;Moa, T.;Mochizuki, K.;Mogg, P.;Mohapatra, S.;Molander, S.;Moles-Valls, R.;Mondragon, M. C.;Mönig, K.;Monk, J.;Monnier, E.;Montalbano, A.;Montejo Berlingen, J.;Monticelli, F.;Monzani, S.;Morange, N.;Moreno, D.;Moreno Llácer, M.;Morettini, P.;Morgenstern, M.;Morgenstern, S.;Mori, D.;Morii, M.;Morinaga, M.;Morisbak, V.;Morley, A. K.;Mornacchi, G.;Morris, A. P.;Morris, J. D.;Morvaj, L.;Moschovakos, P.;Mosidze, M.;Moss, H. J.;Moss, J.;Motohashi, K.;Mount, R.;Mountricha, E.;Moyse, E. J. W.;Muanza, S.;Mueller, F.;Mueller, J.;Mueller, R. S. P.;Muenstermann, D.;Mullier, G. A.;Munoz Sanchez, F. J.;Murin, P.;Murray, W. J.;Murrone, A.;Muškinja, M.;Mwewa, C.;Myagkov, A. G.;Myers, J.;Myska, M.;Nachman, B. P.;Nackenhorst, O.;Nagai, K.;Nagano, K.;Nagasaka, Y.;Nagel, M.;Nagy, E.;Nairz, A. M.;Nakahama, Y.;Nakamura, K.;Nakamura, T.;Nakano, I.;Nanjo, H.;Napolitano, F.;Naranjo Garcia, R. F.;Narayan, R.;Narrias Villar, D. I.;Naryshkin, I.;Naumann, T.;Navarro, G.;Nayyar, R.;Neal, H. A.;Nechaeva, P. Y.;Neep, T. J.;Negri, A.;Negrini, M.;Nektarijevic, S.;Nellist, C.;Nelson, M. E.;Nemecek, S.;Nemethy, P.;Nessi, M.;Neubauer, M. S.;Neumann, M.;Newman, P. R.;Ng, T. Y.;Ng, Y. S.;Ng, Y. W. Y.;Nguyen, H. D. N.;Nguyen Manh, T.;Nibigira, E.;Nickerson, R. B.;Nicolaidou, R.;Nielsen, D. S.;Nielsen, J.;Nikiforou, N.;Nikolaenko, V.;Nikolic-Audit, I.;Nikolopoulos, K.;Nilsson, P.;Nindhito, H. R.;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.;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.;Orellana, G. E.;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.;Park, T. H.;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. E.;Peyaud, A.;Pezoa, R.;Pham, T.;Phillips, F. H.;Phillips, P. W.;Phipps, M. W.;Piacquadio, G.;Pianori, E.;Picazio, A.;Pickles, R. H.;Piegaia, R.;Pilcher, J. E.;Pilkington, A. D.;Pinamonti, M.;Pinfold, J. L.;Pitt, M.;Pizzimento, L.;Pleier, M. -A.;Pleskot, V.;Plotnikova, E.;Pluth, D.;Podberezko, P.;Poettgen, R.;Poggi, R.;Poggioli, L.;Pogrebnyak, I.;Pohl, D.;Pokharel, I.;Polesello, G.;Poley, A.;Policicchio, A.;Polifka, R.;Polini, A.;Pollard, C. S.;Polychronakos, V.;Ponomarenko, D.;Pontecorvo, L.;Popeneciu, G. A.;Portillo Quintero, D. M.;Pospisil, S.;Potamianos, K.;Potrap, I. 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2019-01-01
Abstract
A search for new particles decaying into a pair of top quarks is performed using proton-proton collision data recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of root s = 13 TeV corresponding to an integrated luminosity of 36.1 fb(-1). Events consistent with top-quark pair production and the fully hadronic decay mode of the top quarks are selected by requiring multiple high transverse momentum jets including those containing b-hadrons. Two analysis techniques, exploiting dedicated top-quark pair reconstruction in different kinematic regimes, are used to optimize the search sensitivity to new hypothetical particles over a wide mass range. The invariant mass distribution of the two reconstructed top-quark candidates is examined for resonant production of new particles with various spins and decay widths. No significant deviation from the Standard Model prediction is observed and limits are set on the production cross-section times branching fraction for new hypothetical Z' bosons, dark-matter mediators, Kaluza-Klein gravitons and Kaluza-Klein gluons. By comparing with the predicted production cross sections, the Z' boson in the topcolor-assisted-technicolor model is excluded for masses up to 3.1-3.6 TeV, the dark-matter mediators in a simplified framework are excluded in the mass ranges from 0.8 to 0.9 TeV and from 2.0 to 2.2 TeV, and the Kaluza-Klein gluon is excluded for masses up to 3.4 TeV, depending on the decay widths of the particles.
Aaboud, M., Aad, G., Abbott, B., Abbott, D. ., Abdinov, O., Abeloos, B., et al. (2019). Search for heavy particles decaying into a top-quark pair in the fully hadronic final state in
pp
collisions at
s=13 TeV
with the ATLAS detector. PHYSICAL REVIEW D, 99(9) [10.1103/PhysRevD.99.092004].
Aaboud, M; Aad, G; Abbott, B; Abbott, D ; Abdinov, O; Abeloos, B; Abhayasinghe, D ; Abidi, S ; Abouzeid, O ; Abraham, N ; Abramowicz, H; Abreu, H; Abulaiti, Y; Acharya, B ; Adachi, S; Adam, L; Adamczyk, L; Adamek, L; Adelman, J; Adersberger, M; Adiguzel, A; Adye, T; Affolder, A ; Afik, Y; Agheorghiesei, C; Aguilar-Saavedra, J ; Ahmadov, F; Aielli, G; Akatsuka, S; Åkesson, T ; Akilli, E; Akimov, A ; Alberghi, G ; Albert, J; Albicocco, P; Alconada Verzini, M ; Alderweireldt, S; Aleksa, M; Aleksandrov, I ; Alexa, C; Alexandre, D; Alexopoulos, T; Alhroob, M; Ali, B; Alimonti, G; Alison, J; Alkire, S ; Allaire, C; Allbrooke, B ; Allen, B ; Allport, P ; Aloisio, A; Alonso, A; Alonso, F; Alpigiani, C; Alshehri, A ; Alstaty, M ; Alvarez Gonzalez, B; Álvarez Piqueras, D; Alviggi, M ; Amadio, B ; Amaral Coutinho, Y; Ambler, A; Ambroz, L; Amelung, C; Amidei, D; Amor Dos Santos, S ; Amoroso, S; Amrouche, C ; An, F; Anastopoulos, C; Ancu, L ; Andari, N; Andeen, T; Anders, C ; Anders, J ; Anderson, K ; 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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.
