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Catalogo dei prodotti della ricerca
Angular correlations between heavy-flavor decay electrons and charged particles at midrapidity
(jηj < 0.8) are measured in p-Pb collisions at ffiffiffiffiffiffiffiffi
s NN
p ¼ 5.02 TeV. The analysis is carried out for the
0%–20% (high) and 60%–100% (low) multiplicity ranges. The jet contribution in the correlation distribution
from high-multiplicity events is removed by subtracting the distribution from low-multiplicity events.
An azimuthal modulation remains after removing the jet contribution, similar to previous observations in
two-particle angular correlation measurements for light-flavor hadrons. A Fourier decomposition of the
modulation results in a positive second-order coefficient (v2) for heavy-flavor decay electrons in the
transverse momentum interval 1.5 < pT < 4 GeV=c in high-multiplicity events, with a significance larger
than 5σ. The results are compared with those of charged particles at midrapidity and those of inclusive muons
at forward rapidity. The v2 measurement of open heavy-flavor particles at midrapidity in small collision
systems could provide crucial information to help interpret the anisotropies observed in such systems
Angular correlations between heavy-flavor decay electrons and charged particles at midrapidity (|η|<0.8) are measured in p-Pb collisions at √sNN=5.02TeV. The analysis is carried out for the 0%–20% (high) and 60%–100% (low) multiplicity ranges. The jet contribution in the correlation distribution from high-multiplicity events is removed by subtracting the distribution from low-multiplicity events. An azimuthal modulation remains after removing the jet contribution, similar to previous observations in two-particle angular correlation measurements for light-flavor hadrons. A Fourier decomposition of the modulation results in a positive second-order coefficient (v2) for heavy-flavor decay electrons in the transverse momentum interval 1.5<4 GeV/c in high-multiplicity events, with a significance larger than 5σ. The results are compared with those of charged particles at midrapidity and those of inclusive muons at forward rapidity. The v2 measurement of open heavy-flavor particles at midrapidity in small collision systems could provide crucial information to help interpret the anisotropies observed in such systems.
Azimuthal Anisotropy of Heavy-Flavor Decay Electrons in p -Pb Collisions at sNN =5.02 TeV / Acharya, S., Adamová, D., Adolfsson, J., Aggarwal, M.M., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahn, S.U., Aiola, S., Akindinov, A., Al-Turany, M., Alam, S.N., Albuquerque, D.S.D., Aleksandrov, D., Alessandro, B., Alfaro Molina, R., Ali, Y., Alici, A., Alkin, A., et al.. - In: PHYSICAL REVIEW LETTERS. - ISSN 0031-9007. - 122:7(2019). [10.1103/PhysRevLett.122.072301]
Azimuthal Anisotropy of Heavy-Flavor Decay Electrons in p -Pb Collisions at sNN =5.02 TeV
Acharya, S.;Adamová, D.;Adolfsson, J.;Aggarwal, M. M.;Aglieri Rinella, G.;Agnello, M.;Agrawal, N.;Ahammed, Z.;Ahn, S. U.;Aiola, S.;Akindinov, A.;Al-Turany, M.;Alam, S. N.;Albuquerque, D. S. D.;Aleksandrov, D.;Alessandro, B.;Alfaro Molina, R.;Ali, Y.;Alici, A.;Alkin, A.;Alme, J.;Alt, T.;Altenkamper, L.;Altsybeev, I.;Anaam, M. N.;Andrei, C.;Andreou, D.;Andrews, H. A.;Andronic, A.;Angeletti, M.;Anguelov, V.;Anson, C.;Antičić, T.;Antinori, F.;Antonioli, P.;Anwar, R.;Apadula, N.;Aphecetche, L.;Appelshäuser, H.;Arcelli, S.;Arnaldi, R.;Arnold, O. W.;Arsene, I. C.;Arslandok, M.;Augustinus, A.;Averbeck, R.;Azmi, M. D.;Badalà, A.;Baek, Y. W.;Bagnasco, S.;Bailhache, R.;Bala, R.;Baldisseri, A.;Ball, M.;Baral, R. C.;Barbano, A. M.;Barbera, R.;Barile, F.;Barioglio, L.;Barnaföldi, G. G.;Barnby, L. S.;Barret, V.;Bartalini, P.;Barth, K.;Bartsch, E.;Bastid, N.;Basu, S.;Batigne, G.;Batyunya, B.;Batzing, P. C.;Bazo Alba, J. L.;Bearden, I. G.;Beck, H.;Bedda, C.;Behera, N. K.;Belikov, I.;Bellini, F.;Bello Martinez, H.;Bellwied, R.;Beltran, L. G. E.;Belyaev, V.;Bencedi, G.;Beole, S.;Bercuci, A.;Berdnikov, Y.;Berenyi, D.;Bertens, R. A.;Berzano, D.;Betev, L.;Bhaduri, P. P.;Bhasin, A.;Bhat, I. R.;Bhatt, H.;Bhattacharjee, B.;Bhom, J.;Bianchi, A.;Bianchi, L.;Bianchi, N.;Bielčík, J.;Bielčíková, J.;Bilandzic, A.;Biro, G.;Biswas, R.;Biswas, S.;Blair, J. T.;Blau, D.;Blume, C.;Boca, G.;Bock, F.;Bogdanov, A.;Boldizsár, L.;Bombara, M.;Bonomi, G.;Bonora, M.;Borel, H.;Borissov, A.;Borri, M.;Botta, E.;Bourjau, C.;Bratrud, L.;Braun-Munzinger, P.;Bregant, M.;Broker, T. A.;Broz, M.;Brucken, E. J.;Bruna, E.;Bruno, G. E.;Budnikov, D.;Buesching, H.;Bufalino, S.;Buhler, P.;Buncic, P.;Busch, O.;Buthelezi, Z.;Butt, J. B.;Buxton, J. T.;Cabala, J.;Caffarri, D.;Caines, H.;Caliva, A.;Calvo Villar, E.;Camacho, R. S.;Camerini, P.;Capon, A. A.;Carena, F.;Carena, W.;Carnesecchi, F.;Castillo Castellanos, J.;Castro, A. J.;Casula, E. A. R.;Ceballos Sanchez, C.;Chandra, S.;Chang, B.;Chang, W.;Chapeland, S.;Chartier, M.;Chattopadhyay, S.;Chattopadhyay, S.;Chauvin, A.;Cheshkov, C.;Cheynis, B.;Chibante Barroso, V.;Chinellato, D. D.;Cho, S.;Chochula, P.;Chowdhury, T.;Christakoglou, P.;Christensen, C. H.;Christiansen, P.;Chujo, T.;Chung, S. U.;Cicalo, C.;Cifarelli, L.;Cindolo, F.;Cleymans, J.;Colamaria, F.;Colella, D.;Collu, A.;Colocci, M.;Concas, M.;Conesa Balbastre, G.;Conesa Del Valle, Z.;Contreras, J. G.;Cormier, T. M.;Corrales Morales, Y.;Cortese, P.;Cosentino, M. R.;Costa, F.;Costanza, S.;Crkovská, J.;Crochet, P.;Cuautle, E.;Cunqueiro, L.;Dahms, T.;Dainese, A.;Dani, S.;Danisch, M. C.;Danu, A.;Das, D.;Das, I.;Das, S.;Dash, A.;Dash, S.;De, S.;De Caro, A.;De Cataldo, G.;De Conti, C.;De Cuveland, J.;De Falco, A.;De Gruttola, D.;De Marco, N.;De Pasquale, S.;De Souza, R. D.;Degenhardt, H. F.;Deisting, A.;Deloff, A.;Delsanto, S.;Deplano, C.;Dhankher, P.;Di Bari, D.;Di Mauro, A.;Di Ruzza, B.;Diaz, R. A.;Dietel, T.;Dillenseger, P.;Ding, Y.;Divià, R.;Djuvsland, Ø.;Dobrin, A.;Domenicis Gimenez, D.;Dönigus, B.;Dordic, O.;Doremalen, L. V. R.;Dubey, A. K.;Dubla, A.;Ducroux, L.;Dudi, S.;Duggal, A. K.;Dukhishyam, M.;Dupieux, P.;Ehlers, R. J.;Elia, D.;Endress, E.;Engel, H.;Epple, E.;Erazmus, B.;Erhardt, F.;Ersdal, M. R.;Espagnon, B.;Eulisse, G.;Eum, J.;Evans, D.;Evdokimov, S.;Fabbietti, L.;Faggin, M.;Faivre, J.;Fantoni, A.;Fasel, M.;Feldkamp, L.;Feliciello, A.;Feofilov, G.;Fernández Téllez, A.;Ferretti, A.;Festanti, A.;Feuillard, V. J. G.;Figiel, J.;Figueredo, M. A. S.;Filchagin, S.;Finogeev, D.;Fionda, F. M.;Fiorenza, G.;Flor, F.;Floris, M.;Foertsch, S.;Foka, P.;Fokin, S.;Fragiacomo, E.;Francescon, A.;Francisco, A.;Frankenfeld, U.;Fronze, G. G.;Fuchs, U.;Furget, C.;Furs, A.;Fusco Girard, M.;Gaardhøje, J. J.;Gagliardi, M.;Gago, A. M.;Gajdosova, K.;Gallio, M.;Galvan, C. D.;Ganoti, P.;Garabatos, C.;Garcia-Solis, E.;Garg, K.;Gargiulo, C.;Gasik, P.;Gauger, E. F.;Gay Ducati, M. B.;Germain, M.;Ghosh, J.;Ghosh, P.;Ghosh, S. K.;Gianotti, P.;Giubellino, P.;Giubilato, P.;Glässel, P.;Goméz Coral, D. M.;Gomez Ramirez, A.;Gonzalez, V.;González-Zamora, P.;Gorbunov, S.;Görlich, L.;Gotovac, S.;Grabski, V.;Graczykowski, L. K.;Graham, K. L.;Greiner, L.;Grelli, A.;Grigoras, C.;Grigoriev, V.;Grigoryan, A.;Grigoryan, S.;Gronefeld, J. M.;Grosa, F.;Grosse-Oetringhaus, J. F.;Grosso, R.;Guernane, R.;Guerzoni, B.;Guittiere, M.;Gulbrandsen, K.;Gunji, T.;Gupta, A.;Gupta, R.;Guzman, I. B.;Haake, R.;Habib, M. K.;Hadjidakis, C.;Hamagaki, H.;Hamar, G.;Hamid, M.;Hamon, J. C.;Hannigan, R.;Haque, M. R.;Harlenderova, A.;Harris, J. W.;Harton, A.;Hassan, H.;Hatzifotiadou, D.;Hayashi, S.;Heckel, S. T.;Hellbär, E.;Helstrup, H.;Herghelegiu, A.;Hernandez, E. G.;Herrera Corral, G.;Herrmann, F.;Hetland, K. F.;Hilden, T. E.;Hillemanns, H.;Hills, C.;Hippolyte, B.;Hohlweger, B.;Horak, D.;Hornung, S.;Hosokawa, R.;Hota, J.;Hristov, P.;Huang, C.;Hughes, C.;Huhn, P.;Humanic, T. J.;Hushnud, H.;Hussain, N.;Hussain, T.;Hutter, D.;Hwang, D. S.;Iddon, J. P.;Iga Buitron, S. A.;Ilkaev, R.;Inaba, M.;Ippolitov, M.;Islam, M. S.;Ivanov, M.;Ivanov, V.;Izucheev, V.;Jacak, B.;Jacazio, N.;Jacobs, P. M.;Jadhav, M. B.;Jadlovska, S.;Jadlovsky, J.;Jaelani, S.;Jahnke, C.;Jakubowska, M. J.;Janik, M. A.;Jena, C.;Jercic, M.;Jevons, O.;Jimenez Bustamante, R. T.;Jin, M.;Jones, P. G.;Jusko, A.;Kalinak, P.;Kalweit, A.;Kang, J. H.;Kaplin, V.;Kar, S.;Karasu Uysal, A.;Karavichev, O.;Karavicheva, T.;Karczmarczyk, P.;Karpechev, E.;Kebschull, U.;Keidel, R.;Keijdener, D. L. D.;Keil, M.;Ketzer, B.;Khabanova, Z.;Khan, A. M.;Khan, S.;Khan, S. A.;Khanzadeev, A.;Kharlov, Y.;Khatun, A.;Khuntia, A.;Kielbowicz, M. M.;Kileng, B.;Kim, B.;Kim, D.;Kim, D. J.;Kim, E. J.;Kim, H.;Kim, J. S.;Kim, J.;Kim, M.;Kim, S.;Kim, T.;Kim, T.;Kirsch, S.;Kisel, I.;Kiselev, S.;Kisiel, A.;Klay, J. L.;Klein, C.;Klein, J.;Klein-Bösing, C.;Klewin, S.;Kluge, A.;Knichel, M. L.;Knospe, A. G.;Kobdaj, C.;Kofarago, M.;Köhler, M. K.;Kollegger, T.;Kondratyeva, N.;Kondratyuk, E.;Konevskikh, A.;Konopka, P. J.;Konyushikhin, M.;Kovalenko, O.;Kovalenko, V.;Kowalski, M.;Králik, I.;Kravčáková, A.;Kreis, L.;Krivda, M.;Krizek, F.;Krüger, M.;Kryshen, E.;Krzewicki, M.;Kubera, A. M.;Kučera, V.;Kuhn, C.;Kuijer, P. G.;Kumar, J.;Kumar, L.;Kumar, S.;Kundu, S.;Kurashvili, P.;Kurepin, A.;Kurepin, A. B.;Kuryakin, A.;Kushpil, S.;Kvapil, J.;Kweon, M. J.;Kwon, Y.;La Pointe, S. L.;La Rocca, P.;Lai, Y. S.;Lakomov, I.;Langoy, R.;Lapidus, K.;Lardeux, A.;Larionov, P.;Laudi, E.;Lavicka, R.;Lea, R.;Leardini, L.;Lee, S.;Lehas, F.;Lehner, S.;Lehrbach, J.;Lemmon, R. C.;León Monzón, I.;Lévai, P.;Li, X.;Li, X. L.;Lien, J.;Lietava, R.;Lim, B.;Lindal, S.;Lindenstruth, V.;Lindsay, S. W.;Lippmann, C.;Lisa, M. A.;Litichevskyi, V.;Liu, A.;Ljunggren, H. M.;Llope, W. J.;Lodato, D. F.;Loginov, V.;Loizides, C.;Loncar, P.;Lopez, X.;López Torres, E.;Lowe, A.;Luettig, P.;Luhder, J. R.;Lunardon, M.;Luparello, G.;Lupi, M.;Maevskaya, A.;Mager, M.;Mahmood, S. M.;Maire, A.;Majka, R. D.;Malaev, M.;Malik, Q. W.;Malinina, L.;Mal'Kevich, D.;Malzacher, P.;Mamonov, A.;Manko, V.;Manso, F.;Manzari, V.;Mao, Y.;Marchisone, M.;Mareš, J.;Margagliotti, G. V.;Margotti, A.;Margutti, J.;Marín, A.;Markert, C.;Marquard, M.;Martin, N. A.;Martinengo, P.;Martinez, J. L.;Martínez, M. I.;Martínez García, G.;Martinez Pedreira, M.;Masciocchi, S.;Masera, M.;Masoni, A.;Massacrier, L.;Masson, E.;Mastroserio, A.;Mathis, A. M.;Matuoka, P. F. T.;Matyja, A.;Mayer, C.;Mazzilli, M.;Mazzoni, M. A.;Meddi, F.;Melikyan, Y.;Menchaca-Rocha, A.;Meninno, E.;Mercado Pérez, J.;Meres, M.;Meza, C. S.;Mhlanga, S.;Miake, Y.;Micheletti, L.;Mieskolainen, M. M.;Mihaylov, D. L.;Mikhaylov, K.;Mischke, A.;Mishra, A. N.;Miśkowiec, D.;Mitra, J.;Mitu, C. M.;Mohammadi, N.;Mohanty, A. P.;Mohanty, B.;Mohisin Khan, M.;Moreira De Godoy, D. A.;Moreno, L. A. P.;Moretto, S.;Morreale, A.;Morsch, A.;Mrnjavac, T.;Muccifora, V.;Mudnic, E.;Mühlheim, D.;Muhuri, S.;Mukherjee, M.;Mulligan, J. D.;Munhoz, M. G.;Münning, K.;Munoz, M. I. A.;Munzer, R. H.;Murakami, H.;Murray, S.;Musa, L.;Musinsky, J.;Myers, C. J.;Myrcha, J. W.;Naik, B.;Nair, R.;Nandi, B. K.;Nania, R.;Nappi, E.;Narayan, A.;Naru, M. U.;Nassirpour, A. F.;Natal Da Luz, H.;Nattrass, C.;Navarro, S. R.;Nayak, K.;Nayak, R.;Nayak, T. K.;Nazarenko, S.;Negrao De Oliveira, R. A.;Nellen, L.;Nesbo, S. V.;Neskovic, G.;Ng, F.;Nicassio, M.;Niedziela, J.;Nielsen, B. S.;Nikolaev, S.;Nikulin, S.;Nikulin, V.;Noferini, F.;Nomokonov, P.;Nooren, G.;Noris, J. C. C.;Norman, J.;Nyanin, A.;Nystrand, J.;Oh, H.;Ohlson, A.;Oleniacz, J.;Oliveira Da Silva, A. C.;Oliver, M. H.;Onderwaater, J.;Oppedisano, C.;Orava, R.;Oravec, M.;Ortiz Velasquez, A.;Oskarsson, A.;Otwinowski, J.;Oyama, K.;Pachmayer, Y.;Pacik, V.;Pagano, D.;Paić, G.;Palni, P.;Pan, J.;Pandey, A. K.;Panebianco, S.;Papikyan, V.;Pareek, P.;Park, J.;Parkkila, J. E.;Parmar, S.;Passfeld, A.;Pathak, S. P.;Patra, R. N.;Paul, B.;Pei, H.;Peitzmann, T.;Peng, X.;Pereira, L. G.;Pereira Da Costa, H.;Peresunko, D.;Perez Lezama, E.;Peskov, V.;Pestov, Y.;Petráček, V.;Petrovici, M.;Petta, C.;Pezzi, R. P.;Piano, S.;Pikna, M.;Pillot, P.;Pimentel, L. O. D. L.;Pinazza, O.;Pinsky, L.;Pisano, S.;Piyarathna, D. B.;Płoskoń, M.;Planinic, M.;Pliquett, F.;Pluta, J.;Pochybova, S.;Podesta-Lerma, P. L. M.;Poghosyan, M. G.;Polichtchouk, B.;Poljak, N.;Poonsawat, W.;Pop, A.;Poppenborg, H.;Porteboeuf-Houssais, S.;Pozdniakov, V.;Prasad, S. K.;Preghenella, R.;Prino, F.;Pruneau, C. A.;Pshenichnov, I.;Puccio, M.;Punin, V.;Putschke, J.;Raha, S.;Rajput, S.;Rak, J.;Rakotozafindrabe, A.;Ramello, L.;Rami, F.;Raniwala, R.;Raniwala, S.;Räsänen, S. S.;Rascanu, B. T.;Ratza, V.;Ravasenga, I.;Read, K. F.;Redlich, K.;Rehman, A.;Reichelt, P.;Reidt, F.;Ren, X.;Renfordt, R.;Reshetin, A.;Revol, J. -P.;Reygers, K.;Riabov, V.;Richert, T.;Richter, M.;Riedler, P.;Riegler, W.;Riggi, F.;Ristea, C.;Rode, S. P.;Rodríguez Cahuantzi, M.;Røed, K.;Rogalev, R.;Rogochaya, E.;Rohr, D.;Röhrich, D.;Rokita, P. S.;Ronchetti, F.;Rosas, E. D.;Roslon, K.;Rosnet, P.;Rossi, A.;Rotondi, A.;Roukoutakis, F.;Roy, C.;Roy, P.;Rueda, O. V.;Rui, R.;Rumyantsev, B.;Rustamov, A.;Ryabinkin, E.;Ryabov, Y.;Rybicki, A.;Saarinen, S.;Sadhu, S.;Sadovsky, S.;Šafařík, K.;Saha, S. K.;Sahoo, B.;Sahoo, P.;Sahoo, R.;Sahoo, S.;Sahu, P. K.;Saini, J.;Sakai, S.;Saleh, M. A.;Sambyal, S.;Samsonov, V.;Sandoval, A.;Sarkar, A.;Sarkar, D.;Sarkar, N.;Sarma, P.;Sas, M. H. P.;Scapparone, E.;Scarlassara, F.;Schaefer, B.;Scheid, H. S.;Schiaua, C.;Schicker, R.;Schmidt, C.;Schmidt, H. R.;Schmidt, M. O.;Schmidt, M.;Schmidt, N. V.;Schukraft, J.;Schutz, Y.;Schwarz, K.;Schweda, K.;Scioli, G.;Scomparin, E.;Šefčík, M.;Seger, J. E.;Sekiguchi, Y.;Sekihata, D.;Selyuzhenkov, I.;Senyukov, S.;Serradilla, E.;Sett, P.;Sevcenco, A.;Shabanov, A.;Shabetai, A.;Shahoyan, R.;Shaikh, W.;Shangaraev, A.;Sharma, A.;Sharma, A.;Sharma, M.;Sharma, N.;Sheikh, A. I.;Shigaki, K.;Shimomura, M.;Shirinkin, S.;Shou, Q.;Shtejer, K.;Sibiriak, Y.;Siddhanta, S.;Sielewicz, K. M.;Siemiarczuk, T.;Silvermyr, D.;Simatovic, G.;Simonetti, G.;Singaraju, R.;Singh, R.;Singh, R.;Singhal, V.;Sinha, T.;Sitar, B.;Sitta, M.;Skaali, T. B.;Slupecki, M.;Smirnov, N.;Snellings, R. J. M.;Snellman, T. W.;Song, J.;Soramel, F.;Sorensen, S.;Sozzi, F.;Sputowska, I.;Stachel, J.;Stan, I.;Stankus, P.;Stenlund, E.;Stocco, D.;Storetvedt, M. M.;Strmen, P.;Suaide, A. A. P.;Sugitate, T.;Suire, C.;Suleymanov, M.;Suljic, M.;Sultanov, R.;Šumbera, M.;Sumowidagdo, S.;Suzuki, K.;Swain, S.;Szabo, A.;Szarka, I.;Tabassam, U.;Takahashi, J.;Tambave, G. J.;Tanaka, N.;Tarhini, M.;Tariq, M.;Tarzila, M. G.;Tauro, A.;Tejeda Muñoz, G.;Telesca, A.;Terrevoli, C.;Teyssier, B.;Thakur, D.;Thakur, S.;Thomas, D.;Thoresen, F.;Tieulent, R.;Tikhonov, A.;Timmins, A. R.;Toia, A.;Topilskaya, N.;Toppi, M.;Torales-Acosta, F.;Torres, S. R.;Tripathy, S.;Trogolo, S.;Trombetta, G.;Tropp, L.;Trubnikov, V.;Trzaska, W. H.;Trzcinski, T. P.;Trzeciak, B. A.;Tsuji, T.;Tumkin, A.;Turrisi, R.;Tveter, T. S.;Ullaland, K.;Umaka, E. N.;Uras, A.;Usai, G. L.;Utrobicic, A.;Vala, M.;Van Hoorne, J. W.;Van Leeuwen, M.;Vande Vyvre, P.;Varga, D.;Vargas, A.;Vargyas, M.;Varma, R.;Vasileiou, M.;Vasiliev, A.;Vauthier, A.;Vázquez Doce, O.;Vechernin, V.;Veen, A. M.;Vercellin, E.;Vergara Limón, S.;Vermunt, L.;Vernet, R.;Vértesi, R.;Vickovic, L.;Viinikainen, J.;Vilakazi, Z.;Villalobos Baillie, O.;Villatoro Tello, A.;Vinogradov, A.;Virgili, T.;Vislavicius, V.;Vodopyanov, A.;Völkl, M. A.;Voloshin, K.;Voloshin, S. A.;Volpe, G.;Von Haller, B.;Vorobyev, I.;Voscek, D.;Vranic, D.;Vrláková, J.;Wagner, B.;Wang, H.;Wang, M.;Watanabe, Y.;Weber, M.;Weber, S. G.;Wegrzynek, A.;Weiser, D. F.;Wenzel, S. C.;Wessels, J. P.;Westerhoff, U.;Whitehead, A. M.;Wiechula, J.;Wikne, J.;Wilk, G.;Wilkinson, J.;Willems, G. A.;Williams, M. C. S.;Willsher, E.;Windelband, B.;Witt, W. E.;Xu, R.;Yalcin, S.;Yamakawa, K.;Yano, S.;Yin, Z.;Yokoyama, H.;Yoo, I. -K.;Yoon, J. H.;Yurchenko, V.;Zaccolo, V.;Zaman, A.;Zampolli, C.;Zanoli, H. J. C.;Zardoshti, N.;Zarochentsev, A.;Závada, P.;Zaviyalov, N.;Zbroszczyk, H.;Zhalov, M.;Zhang, X.;Zhang, Y.;Zhang, Z.;Zhao, C.;Zherebchevskii, V.;Zhigareva, N.;Zhou, D.;Zhou, Y.;Zhou, Z.;Zhu, H.;Zhu, J.;Zhu, Y.;Zichichi, A.;Zimmermann, M. B.;Zinovjev, G.;Zmeskal, J.;Zou, S.
2019
Abstract
Angular correlations between heavy-flavor decay electrons and charged particles at midrapidity
(jηj < 0.8) are measured in p-Pb collisions at ffiffiffiffiffiffiffiffi
s NN
p ¼ 5.02 TeV. The analysis is carried out for the
0%–20% (high) and 60%–100% (low) multiplicity ranges. The jet contribution in the correlation distribution
from high-multiplicity events is removed by subtracting the distribution from low-multiplicity events.
An azimuthal modulation remains after removing the jet contribution, similar to previous observations in
two-particle angular correlation measurements for light-flavor hadrons. A Fourier decomposition of the
modulation results in a positive second-order coefficient (v2) for heavy-flavor decay electrons in the
transverse momentum interval 1.5 < pT < 4 GeV=c in high-multiplicity events, with a significance larger
than 5σ. The results are compared with those of charged particles at midrapidity and those of inclusive muons
at forward rapidity. The v2 measurement of open heavy-flavor particles at midrapidity in small collision
systems could provide crucial information to help interpret the anisotropies observed in such systems
Angular correlations between heavy-flavor decay electrons and charged particles at midrapidity (|η|<0.8) are measured in p-Pb collisions at √sNN=5.02TeV. The analysis is carried out for the 0%–20% (high) and 60%–100% (low) multiplicity ranges. The jet contribution in the correlation distribution from high-multiplicity events is removed by subtracting the distribution from low-multiplicity events. An azimuthal modulation remains after removing the jet contribution, similar to previous observations in two-particle angular correlation measurements for light-flavor hadrons. A Fourier decomposition of the modulation results in a positive second-order coefficient (v2) for heavy-flavor decay electrons in the transverse momentum interval 1.5<4 GeV/c in high-multiplicity events, with a significance larger than 5σ. The results are compared with those of charged particles at midrapidity and those of inclusive muons at forward rapidity. The v2 measurement of open heavy-flavor particles at midrapidity in small collision systems could provide crucial information to help interpret the anisotropies observed in such systems.
quark gluon plasma
01 Pubblicazione su rivista::01a Articolo in rivista
Azimuthal Anisotropy of Heavy-Flavor Decay Electrons in p -Pb Collisions at sNN =5.02 TeV / Acharya, S., Adamová, D., Adolfsson, J., Aggarwal, M.M., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahn, S.U., Aiola, S., Akindinov, A., Al-Turany, M., Alam, S.N., Albuquerque, D.S.D., Aleksandrov, D., Alessandro, B., Alfaro Molina, R., Ali, Y., Alici, A., Alkin, A., et al.. - In: PHYSICAL REVIEW LETTERS. - ISSN 0031-9007. - 122:7(2019). [10.1103/PhysRevLett.122.072301]
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11573/1469777
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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.
