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Cleymans, Jean Willy Andre ; Coccetti, F. ; Coffin, J.-P. ; Coli, S. ; Conesa Balbastre, Gustavo ; Conesa del Valle, Zaida ; Constantin, P. ; Contin, Giacomo ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortés Maldonado, Ismael ; Cortese, Pietro ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Cotallo, M.E. ; Crescio, E. ; Crochet, Philippe ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; Erasmo, G.D. ; Dainese, Andrea ; Dalsgaard, H.H. ; Danu, Andrea ; Das, Debasish ; Das, Indranil ; Dash, Ajay Kumar ; Dash, Sadhana ; De, Sudipan ; De Azevedo Moregula, A. ; de Barros, G.O.V. ; De Caro, Annalisa ; De Cataldo, Giacinto ; Cuveland, Jan de ; De Falco, Alessandro ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; De Remigis, R. ; de Rooij, R. ; Delagrange, H. ; Delgado Mercado, Y. ; Dellacasa, G. ; Deloff, Andrzej ; Demanov, V. ; Dénes, Ervin Sandor ; Deppman, A. ; Di Bari, Domenico ; Di Giglio, C. ; Di Liberto, S. ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Dietel, Thomas ; Divià, Roberto ; Djuvsland, Øystein ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Domínguez, I. ; Dönigus, Benjamin ; Dordic, Olja ; Driga, O. ; Dubey, Anand Kumar ; Dubuisson, J. ; Ducroux, Laurent ; Dupieux, Pascal ; Dutta Majumdar, A.K. ; Dutta Majumdar, M.R. ; Elia, Domenico ; Emschermann, D. ; Engel, Heiko ; Erdal, H.A. ; Espagnon, Bruno ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evrard, S. ; Eyyubova, Gyulnara ; Fabjan, C.W. ; Fabris, Daniela ; Faivre, Julien ; Falchieri, D. ; Fantoni, Alessandra ; Fasel, Markus ; Fearick, R. ; Fedunov, A. ; Fehlker, D. ; Fekete, V. ; Felea, Daniel ; Feofilov, Grigori A. ; Fernández Téllez, Arturo ; Ferretti, Alessandro ; Ferretti, R. ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Fini, R. ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Fragkiadakis, M. ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furano, F. ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhøje, Jens Jørgen ; Gadrat, S. ; Gagliardi, Martino ; Gago, A. ; Gallio, Mauro ; Ganoti, Paraskevi ; Garabatos, Chilo ; Gemme, R. ; Gerhard, J. ; Germain, Marie ; Geuna, C. ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, B. ; Ghosh, Premomoy ; Girard, M.R. ; Giraudo, G. ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glässel, Peter ; Gomez, R. ; González Trueba, Laura Helena ; González Zamora, Pedro ; González Santos, H. ; Gorbunov, Sergey ; Gotovac, Sven ; Grabski, Varlen ; Grajcarek, R. ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoriev, Vladislav A. ; Grigoryan, Ara ; Grigoryan, Smbat ; Grinyov, Boris V. ; Grion, Nevio ; Gros, P. ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Grosso, Raffaele ; Guber, Fedor ; Guernane, Rachid ; Guerra Gutierrez, C. ; Guerzoni, Barbara ; Gulbrandsen, Kristjan Herlache ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Gutbrod, H. ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Harris, John W. ; Hartig, M. ; Hasch, D. ; Hasegan, D. ; Hatzifotiadou, Despina ; Hayrapetyan, A. ; Heide, Markus ; Heinz, Mark Thomas ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Hernández, C. ; Herrera Corral, Gerardo Antonio ; Herrmann, Norbert ; Hetland, Kristin Fanebust ; Hicks, B. ; Hille, P.T. ; Hippolyte, Boris ; Horaguchi, T. ; Hori, Y. ; Hristov, Peter ; Hřivnáčová, I. ; Huang, M. ; Huber, S. ; Humanic, Thomas J. ; Hwang, D.S. ; Ichou, R. ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Incani, E. ; Innocenti, Gian Michele ; Innocenti, P.G. ; Ippolitov, Mikhail ; Irfan, M. ; Ivan, C. ; Ivanov, A. ; Ivanov, Marian ; Ivanov, V. ; Jacholkowski, Adam Wlodzimierz ; Jacobs, Peter Martin ; Jancurová, L. ; Jangal, S. ; Janik, R. ; Jayarathna, S.P. ; Jena, Satyajit ; Jirden, L. ; Jones, Goronwy Tudor ; Jones, Peter Graham ; Jovanović, P. ; Jung, H. ; Jung, W. ; Jusko, Anton ; Kalcher, S. ; Kaliňák, Peter ; Kalisky, M. ; Kalliokoski, T. ; Kalweit, Alexander Philipp ; Kamermans, R. ; Kanaki, K. ; Kang, E. ; Kang, Ju Hwan ; Kaplin, Vladimir ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kazantsev, Andrey ; Kebschull, Udo ; Keidel, Ralf ; Khan, M.M. ; Khanzadeev, Alexei ; Kharlov, Yury ; Kileng, Bjarte ; Kim, D.J. ; Kim, D.S. ; Kim, D.W. ; Kim, H.N. ; Kim, J.H. ; Kim, J.S. ; Kim, M. ; Kim, M. ; Kim, S. ; Kim, S.H. ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kliemant, Michael ; Klovning, A. ; Kluge, Alexander ; Knichel, Michael Linus ; Koch, K. ; Köhler, Markus Konrad ; Kolevatov, R. ; Kolojvari, Anatoly ; Kondratiev, Valery P. ; Kondratyeva, Natalia ; Konevskih, A. ; Kornaś, Ewelina ; Kottachchi Kankanamge Don, C. ; Kour, R. ; Kowalski, Marek ; Kox, Serge ; Kozlov, K. ; Kral, Jiří ; Králik, Ivan ; Kramer, F. ; Kraus, Ingrid ; Krawutschke, T. ; Kretz, Matthias ; Krivda, Marian ; Krumbhorn, D. ; Krus, M. ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucheriaev, Yury ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, Alexey B. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kushpil, V. ; Kweon, Min Jung ; Kwon, Youngil ; La Rocca, Paola ; Ladron de Guevara, Pedro ; Lafage, V. ; Lara Martinez, Camilo Ernesto ; Larsen, D.T. ; Lazzeroni, C. ; Le Bornec, Y. ; Lea, Ramona ; Lee, K.S. ; Lee, S.C. ; Lefèvre, F. ; Lehnert, Jörg ; Leistam, L. ; Lenhardt, M. ; Lenti, Vito ; León Monzón, Ildefonso ; León Vargas, H. ; Lévai, Péter ; Li, X. ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Liu, L. ; Loggins, Vera Renee ; Loginov, Vitaly ; Lohn, S. ; Lohner, D. ; Loizides, Constantinos ; Lopez, Xavier Bernard ; López Noriega, M. ; López Torres, Ernesto ; Løvhøiden, G. ; Lu, X.-G. ; Lüttig, Philipp ; Lunardon, Marcello ; Luparello, Grazia ; Luquin, L. ; Luzzi, C. ; Ma, K. ; Ma, R. ; Madagodahettige-Don, D.M. ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, D.P. ; Maire, Antonin ; Malaev, Mikhail ; Maldonado Cervantes, Ivonne Alicia ; Mal’Kevich, Dmitry ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Mangotra, L. ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Mao, Yaxian ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marín, Ana ; Martashvili, Irakli ; Martinengo, Paolo ; Martínez Hernández, Mario Iván ; Martínez Davalos, A. ; Martínez Garcia, Ginés ; Martynov, Yevgen ; Mas, Alexis Jean-Michel ; Masciocchi, Silvia ; Masera, Massimo ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastromarco, Mario ; Mastroserio, Annalisa ; Matthews, Z.L. ; Matyja, Adam Tomasz ; Mayani, D. ; Mazza, G. ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mendez Lorenzo, P. ; Mercado Pérez, Jorge ; Mereu, P. ; Miake, Yasuo ; Midori, J. ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Miśkowiec, Dariusz Czesław ; Mitu, C. ; Mlynarz, J. ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Monteno, M. ; Montes Prado, Esther ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Müller, H. ; Muhuri, Sanjib ; Munhoz, Marcelo Gameiro ; Munoz, J. ; Musa, Luciano ; Musso, A. ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Navach, F. ; Navin, S. ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nazarov, G. ; Nedosekin, Alexander ; Nendaz, F. ; Newby, J. ; Nicassio, Maria ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikolic, V. ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, B.S. ; Nilsson, M.S. ; Noferini, Francesco ; Nooren, Gerardus ; Novitzky, Norbert ; Nyanin, Alexander ; Nyatha, A. ; Nygaard, C. ; Nystrand, Joakim Ingemar ; Obayashi, H. ; Ochirov, A. ; Oeschler, Helmut ; Oh, Sun Kun ; Oleniacz, Janusz ; Oppedisano, Chiara ; Ortiz Velasquez, Antonio ; 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Inclusive transverse momentum spectra of primary charged particles in Pb–Pb collisions at √sNN=2.76 TeV have been measured by the ALICE Collaboration at the LHC. The data are presented for central and peripheral collisions, corresponding to 0–5% and 70–80% of the hadronic Pb–Pb cross section. The measured charged particle spectra in |η|<0.8 and 0.3<pT<20 GeV/c are compared to the expectation in pp collisions at the same sNN, scaled by the number of underlying nucleon–nucleon collisions. The comparison is expressed in terms of the nuclear modification factor RAA. The result indicates only weak medium effects (RAA≈0.7) in peripheral collisions. In central collisions, RAA reaches a minimum of about 0.14 at pT=6–7 GeV/c and increases significantly at larger pT. The measured suppression of high-pT particles is stronger than that observed at lower collision energies, indicating that a very dense medium is formed in central Pb–Pb collisions at the LHC.
Aamodt, Kenneth ; Abrahantes Quintana, A. ; Adamová, Dagmar ; Adare, A.M. ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agocs, A.G. ; Aguilar Salazar, S. ; Ahammed, Zubayer ; Ahmad, Nazeer ; Ahmad Masoodi, A. ; Ahn, Sang Un ; Akindinov, Alexander ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alfaro Molina, Jose Ruben ; Alici, Andrea ; Alkin, Anton ; Almaráz Aviña, E. ; Alt, Torsten ; Altini, V. ; Altinpinar, Sedat ; Altsybeev, Igor ; Andrei, Cristian ; Andronic, Anton ; Anguelov, Venelin ; Anson, Christopher Daniel ; Antičić, Tome ; Antinori, Federico ; Antonioli, Pietro ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arbor, N. ; Arcelli, Silvia ; Arend, A. ; Armesto, Néstor ; Arnaldi, Roberta ; Aronsson, Tomas Robert ; Arsene, Ionut Cristian ; Asryan, A. ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, T.C. ; Äystö, J. ; Azmi, Mohd Danish ; Bach, Matthias ; Badalà, Angela ; Baek, Yong Wook ; Bagnasco, Stefano ; Bailhache, Raphaëlle ; Bala, Remu ; Baldini Ferroli, Rinaldo ; Baldisseri, Alberto ; Baldit, A. ; Bán, J. ; Barbera, Roberto ; Barile, Francesco ; Barnaföldi, Gergely Gábor ; Barnby, Lee Stuart ; Barret, Valerie ; Bartke, Jerzy ; Basile, Maurizio ; Bastid, Nicole ; Bathen, Bastian ; Batigne, Guillaume ; Batyunya, Boris ; Baumann, C. ; Bearden, Ian Gardner ; Beck, Hans ; Belikov, Iouri ; Bellini, Francesca ; Bellwied, Rene ; Belmont-Moreno, Ernesto ; Beolè, Stefania ; Berceanu, Ionela ; Bercuci, Alexandru ; Berdermann, E. ; Berdnikov, Yaroslav ; Betev, Latchezar ; Bhasin, Anju ; Bhati, Ashok Kumar ; Bianchi, Livio ; Bianchi, Nicola ; Bianchin, Chiara ; Bielčík, Jaroslav ; Bielčíková, Jana ; Bilandzic, Ante ; Biolcati, E. ; Blanc, A. ; Blanco, Fernando ; Blanco, Fernando ; Blau, Dmitry S. ; Blume, Christoph ; Boccioli, M. ; Bock, N. ; Bogdanov, Alexey A. ; Bøggild, Hans ; Bogolyubsky, M. ; Boldizsár, László ; Bombara, Marek ; Bombonati, C. ; Book, Julian ; Borel, Hervé ; Bortolin, C. ; Bose, S. ; Bossú, Francesco ; Botje, Michiel ; Böttger, Stefan ; Boyer, B. ; Braun-Munzinger, Peter ; Bravina, L. ; Bregant, Marco ; Breitner, Timo ; Broz, Michal ; Brun, René ; Bruna, Elena ; Bruno, Giuseppe Eugenio ; Budnikov, Dmitry ; Büsching, Henner ; Busch, Oliver ; Buthelezi, Edith Zinhle ; Caffarri, Davide ; Cai, Xiao ; Caines, Helen Louise ; Calvo Villar, Ernesto ; Camerini, Paolo ; Canoa Roman, Veronica ; Cara Romeo, G. ; Carena, Francesco ; Carena, Wisla ; Carminati, F. ; Casanova Díaz, A. ; Caselle, M. ; Castillo Castellanos, Javier Ernesto ; Catanescu, V. ; Cavicchioli, Costanza ; Cerello, Piergiorgio ; Chang, B. ; Chapeland, Sylvain ; Charvet, Jean-Luc Fernand ; Chattopadhyay, S. ; Chattopadhyay, S. ; Cherney, Michael Gerard ; Cheshkov, Cvetan Valeriev ; Cheynis, Brigitte ; Chiavassa, E. ; Chibante Barroso, Vasco Miguel ; Chinellato, David Dobrigkeit ; Chochula, Peter ; Chojnacki, Marek ; Christakoglou, Panagiotis ; Christensen, Christian Holm ; Christiansen, Peter L. ; Chujo, Tatsuya ; Cicalò, Corrado ; Cifarelli, Luisa ; Cindolo, Federico ; Cleymans, Jean Willy Andre ; Coccetti, F. ; Coffin, J.-P. ; Coli, S. ; Conesa Balbastre, Gustavo ; Conesa del Valle, Zaida ; Constantin, P. ; Contin, Giacomo ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortés Maldonado, Ismael ; Cortese, Pietro ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Cotallo, M.E. ; Crescio, E. ; Crochet, Philippe ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; D’Erasmo, Ginevra ; Dainese, Andrea ; Dalsgaard, H.H. ; Danu, Andrea ; Das, Debasish ; Das, Indranil ; Dash, Ajay Kumar ; Dash, Sadhana ; De, Sudipan ; De Azevedo Moregula, A. ; de Barros, G.O.V. ; De Caro, Annalisa ; De Cataldo, Giacinto ; Cuveland, Jan de ; De Falco, Alessandro ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; De Remigis, R. ; de Rooij, R. ; Delagrange, H. ; Delgado Mercado, Y. ; Dellacasa, G. ; Deloff, Andrzej ; Demanov, V. ; Dénes, Ervin Sandor ; Deppman, A. ; Di Bari, Domenico ; Di Giglio, C. ; Di Liberto, S. ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Dietel, Thomas ; Divià, Roberto ; Djuvsland, Øystein ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Domínguez, I. ; Dönigus, Benjamin ; Dordic, Olja ; Driga, O. ; Dubey, Anand Kumar ; Ducroux, Laurent ; Dupieux, Pascal ; Dutta Majumdar, A.K. ; Dutta Majumdar, M.R. ; Elia, Domenico ; Emschermann, D. ; Engel, Heiko ; Erdal, H.A. ; Espagnon, Bruno ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evrard, S. ; Eyyubova, Gyulnara ; Fabjan, C.W. ; Fabris, Daniela ; Faivre, Julien ; Falchieri, D. ; Fantoni, Alessandra ; Fasel, Markus ; Fearick, R. ; Fedunov, A. ; Fehlker, D. ; Fekete, V. ; Felea, Daniel ; Feofilov, Grigori A. ; Fernández Téllez, Arturo ; Ferretti, Alessandro ; Ferretti, R. ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Fini, R. ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Fragkiadakis, M. ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furano, F. ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhøje, Jens Jørgen ; Gadrat, S. ; Gagliardi, Martino ; Gago, A. ; Gallio, Mauro ; Ganoti, Paraskevi ; Garabatos, Chilo ; Gemme, R. ; Gerhard, J. ; Germain, Marie ; Geuna, C. ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, B. ; Ghosh, Premomoy ; Girard, M.R. ; Giraudo, G. ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glässel, Peter ; Gomez, R. ; González Trueba, Laura Helena ; González Zamora, Pedro ; González Santos, H. ; Gorbunov, Sergey ; Gotovac, Sven ; Grabski, Varlen ; Grajcarek, R. ; Gramling, J.L. ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoriev, Vladislav A. ; Grigoryan, Ara ; Grigoryan, Smbat ; Grinyov, Boris V. ; Grion, Nevio ; Gros, P. ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Grosso, Raffaele ; Guber, Fedor ; Guernane, Rachid ; Guerra Gutierrez, C. ; Guerzoni, Barbara ; Gulbrandsen, Kristjan Herlache ; Gulkanyan, Hrant ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Gutbrod, H. ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Harris, John W. ; Hartig, M. ; Hasch, D. ; Hasegan, D. ; Hatzifotiadou, Despina ; Hayrapetyan, A. ; Heide, Markus ; Heinz, Mark Thomas ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Hernández, C. ; Herrera Corral, Gerardo Antonio ; Herrmann, Norbert ; Hetland, Kristin Fanebust ; Hicks, B. ; Hille, P.T. ; Hippolyte, Boris ; Horaguchi, T. ; Hori, Y. ; Hristov, Peter ; Hřivnáčová, I. ; Huang, M. ; Huber, S. ; Humanic, Thomas J. ; Hwang, D.S. ; Ichou, R. ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Incani, E. ; Innocenti, Gian Michele ; Innocenti, P.G. ; Ippolitov, Mikhail ; Irfan, M. ; Ivan, C. ; Ivanov, A. ; Ivanov, Marian ; Ivanov, V. ; Jacholkowski, Adam Wlodzimierz ; Jacobs, Peter Martin ; Jancurová, L. ; Jangal, S. ; Janik, R. ; Jayarathna, S.P. ; Jena, Satyajit ; Jirden, L. ; Jones, Goronwy Tudor ; Jones, Peter Graham ; Jovanović, P. ; Jung, H. ; Jung, W. ; Jusko, Anton ; Kalcher, S. ; Kaliňák, Peter ; Kalisky, M. ; Kalliokoski, T. ; Kalweit, Alexander Philipp ; Kamermans, R. ; Kanaki, K. ; Kang, E. ; Kang, Ju Hwan ; Kaplin, Vladimir ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kazantsev, Andrey ; Kebschull, Udo ; Keidel, Ralf ; Khan, M.M. ; Khanzadeev, Alexei ; Kharlov, Yury ; Kileng, Bjarte ; Kim, D.J. ; Kim, D.S. ; Kim, D.W. ; Kim, H.N. ; Kim, J.H. ; Kim, J.S. ; Kim, M. ; Kim, M. ; Kim, S. ; Kim, S.H. ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kliemant, Michael ; Klovning, A. ; Kluge, Alexander ; Knichel, Michael Linus ; Koch, K. ; Köhler, Markus Konrad ; Kolevatov, R. ; Kolojvari, Anatoly ; Kondratiev, Valery P. ; Kondratyeva, Natalia ; Konevskih, A. ; Kornaś, Ewelina ; Kottachchi Kankanamge Don, C. ; Kour, R. ; Kowalski, Marek ; Kox, Serge ; Koyithatta Meethaleveedu, Greeshma ; Kozlov, K. ; Kral, Jiří ; Králik, Ivan ; Kramer, F. ; Kraus, Ingrid ; Krawutschke, T. ; Kretz, Matthias ; Krivda, Marian ; Krumbhorn, D. ; Krus, M. ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucheriaev, Yury ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, Alexey B. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kushpil, V. ; Kweon, Min Jung ; Kwon, Youngil ; La Rocca, Paola ; Ladron de Guevara, Pedro ; Lafage, V. ; Lara Martinez, Camilo Ernesto ; Larsen, D.T. ; Lazzeroni, C. ; Le Bornec, Y. ; Lea, Ramona ; Lee, K.S. ; Lee, S.C. ; Lefèvre, F. ; Lehnert, Jörg ; Leistam, L. ; Lenhardt, M. ; Lenti, Vito ; León Monzón, Ildefonso ; León Vargas, H. ; Lévai, Péter ; Li, X. ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Liu, L. ; Loggins, Vera Renee ; Loginov, Vitaly ; Lohn, S. ; Lohner, D. ; Loizides, Constantinos ; Lopez, Xavier Bernard ; López Noriega, M. ; López Torres, Ernesto ; Løvhøiden, G. ; Lu, X.-G. ; Lüttig, Philipp ; Lunardon, Marcello ; Luparello, Grazia ; Luquin, L. ; Luzzi, C. ; Ma, K. ; Ma, R. ; Madagodahettige-Don, D.M. ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, D.P. ; Maire, Antonin ; Malaev, Mikhail ; Maldonado Cervantes, Ivonne Alicia ; Malinina, Liudmila ; Mal’Kevich, Dmitry ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Mangotra, L. ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Mao, Yaxian ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marín, Ana ; Martashvili, Irakli ; Martinengo, Paolo ; Martínez Hernández, Mario Iván ; Martínez Davalos, A. ; Martínez Garcia, Ginés ; Martynov, Yevgen ; Mas, Alexis Jean-Michel ; Masciocchi, Silvia ; Masera, Massimo ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastromarco, Mario ; Mastroserio, Annalisa ; Matthews, Z.L. ; Matyja, Adam Tomasz ; Mayani, D. ; Mazza, G. ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mendez Lorenzo, P. ; Mercado Pérez, Jorge ; Mereu, P. ; Miake, Yasuo ; Midori, J. ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Miśkowiec, Dariusz Czesław ; Mitu, C. ; Mlynarz, J. ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Monteno, M. ; Montes Prado, Esther ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Müller, H. ; Muhuri, Sanjib ; Munhoz, Marcelo Gameiro ; Munoz, J. ; Musa, Luciano ; Musso, A. ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Navach, F. ; Navin, S. ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nazarov, G. ; Nedosekin, Alexander ; Nendaz, F. ; Newby, J. ; Nicassio, Maria ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikolic, V. ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, B.S. ; Nilsson, M.S. ; Noferini, Francesco ; Nooren, Gerardus ; Novitzky, Norbert ; Nyanin, Alexander ; Nyatha, A. ; Nygaard, C. ; Nystrand, Joakim Ingemar ; Obayashi, H. ; Ochirov, A. ; Oeschler, Helmut ; Oh, Sun Kun ; Oleniacz, Janusz ; Oppedisano, Chiara ; Ortiz Velasquez, Antonio ; Ortona, G. ; Oskarsson, Anders Nils Erik ; Ostrowski, P. ; Otterlund, I. ; Otwinowski, Jacek Tomasz ; Ø, G. ; Oyama, Ken ; Ozawa, K. ; Pachmayer, Yvonne C. ; Pachr, Miloš ; Padilla, F. ; Pagano, Paola ; Paić, Guy ; Painke, F. ; Pajares Vales, Carlos ; Pal, S. ; Pal, Susanta Kumar ; Palaha, A. ; Palmeri, A. ; Pappalardo, Giuseppe Salvatore ; Park, WooJin ; Paticchio, Vincenzo ; Pavlinov, A. ; Pawlak, Tomasz Jan ; Peitzmann, Thomas ; Peresunko, Dmitry Yurevich ; Pérez Lara, Carlos Eugenio ; Perini, D. ; Perrino, D. ; Peryt, Wiktor Stanislaw ; Pesci, A. ; Peskov, Vladimir ; Pestov, Yury N. ; Peters, A.J. ; Petráček, Vojtech ; Petris, M. ; Petrov, P. ; Petrovici, Mihai A. ; Petta, Catia ; Piano, Stefano ; Piccotti, A. ; Pikna, Miroslav ; Pillot, Philippe ; Pinazza, Ombretta ; Pinsky, Lawrence ; Pitz, N. ; Piuz, F. ; Piyarathna, Danthasinghe B. ; Platt, R. ; Płoskoń, Mateusz ; Pluta, Jan Marian ; Pocheptsov, T. ; Pochybova, Sona ; Podesta Lerma, Pedro Luis Manuel ; Poghosyan, Martin G. ; Polák, K. ; Polichtchouk, Boris ; Pop, Amalia ; Pospíšil, V. ; Potukuchi, B. ; Prasad, Sidharth Kumar ; Preghenella, Roberto ; Prino, Francesco ; Pruneau, Claude A. ; Pshenichnov, Igor A. ; Puddu, Giovanna ; Pulvirenti, A. ; Punin, Valery ; Putiš, M. ; Putschke, Jörn H. ; Quercigh, E. ; Qvigstad, Henrik ; Rachevski, Alexandre ; Rademakers, A. ; Rademakers, O. ; Radomski, S. ; Räihä, T.S. ; Rak, Jan ; Rakotozafindrabe, Andry Malala ; Ramello, Luciano ; Ramírez Reyes, A. ; Rammler, M. ; Raniwala, Rashmi ; Raniwala, Sudhir ; Räsänen, Sami Sakari ; Read, Kenneth Francis ; Real, Jean-Sébastien ; Redlich, Krzysztof ; Renfordt, Rainer Arno Ernst ; Reolon, Anna Rita ; Reshetin, Andrey ; Rettig, Felix Vincenz ; Revol, Jean-Pierre ; Reygers, Klaus ; Ricaud, H. ; Riccati, L. ; Ricci, Renato Angelo ; Richter, Matthias Rudolph ; Riedler, Petra ; Riegler, Werner ; Riggi, Francesco ; Rivetti, Angelo ; Rodrı́guez Cahuantzi, Mario ; Rohr, David ; Röhrich, Dieter ; Romita, Rosa ; Ronchetti, Federico ; Rosinský, P. ; Rosnet, Philippe ; Rossegger, S. ; Rossi, Andrea ; Roukoutakis, Filimon ; Rousseau, S. ; Roy, Christelle Sophie ; Roy, Pradip Kumar ; Rubio Montero, Antonio Juan ; Rui, Rinaldo ; Rusanov, I. ; Ryabinkin, Evgeny ; Rybicki, Andrzej ; Sadovskiy, Sergey ; Šafařík, Karel ; Sahoo, Raghunath ; Sahu, Pradip Kumar ; Saiz, P. ; Sakai, Shingo ; Sakata, D. ; Salgado, Carlos A. ; Samanta, T. ; Sambyal, Sanjeev Singh ; Samsonov, Vladimir ; Šándor, Ladislav ; Sandoval, Andres ; Sano, Masato ; Sano, S. ; Santo, R. ; Santoro, R. ; Sarkamo, J. ; Saturnini, P. ; Scapparone, Eugenio ; Scarlassara, Fernando ; Scharenberg, Rolf Paul ; Schiaua, Claudiu Cornel ; Schicker, Rainer ; Schmidt, Christian Joachim ; Schmidt, Hans Rudolf ; Schreiner, S. ; Schuchmann, Simone ; Schukraft, Jürgen ; Schutz, Yves Roland ; Schwarz, Kilian ; Schweda, Kai ; Scioli, Gilda ; Scomparin, Enrico ; Scott, P.A. ; Scott, Rebecca Michelle ; Segato, G. ; 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Šumbera, Michal ; Šuša, Tatjana ; Swoboda, D. ; Symons, Timothy James MacNeil ; Toledo, Alejandro Szanto de ; Szarka, Imrich ; Szostak, A. ; Tagridis, C. ; Takahashi, Jun ; Tapia Takaki, Jesus Daniel ; Tauro, Arturo ; Tavlet, M. ; Tejeda Muñoz, Guillermo ; Telesca, Adriana ; Terrevoli, Cristina ; Thäder, Jochen ; Thomas, Deepa ; Thomas, James H. ; Tieulent, Raphael Noel ; Timmins, Anthony Robert ; Tlusty, David ; Toia, Alberica ; Torii, H. ; Toscano, L. ; Tosello, F. ; Traczyk, T. ; Truesdale, David Christopher ; Trzaska, Wladyslaw Henryk ; Tumkin, Alexandr ; Turrisi, Rosario ; Turvey, A.J. ; Tveter, Trine Spedstad ; Ulery, Jason Glyndwr ; Ullaland, Kjetil ; Uras, Antonio ; Urbán, J. ; Urciuoli, G.M. ; Usai, Gianluca ; Vacchi, A. ; Vala, Martin ; Valencia Palomo, Lizardo ; Vallero, Sara ; Kolk, Naomi van der ; Leeuwen, Marco van ; Vyvre, Pierre vande ; Vannucci, L. ; Vargas Treviño, Maria Aurora Diozcora ; Varma, Raghava ; Vasileiou, Maria ; Vasiliev, Andrey ; Vechernin, Vladimir ; Venaruzzo, Massimo ; Vercellin, Ermanno ; Vergara, S. ; Vernet, Renaud ; Verweij, Marta ; Vicković, Linda ; Viesti, Giuseppe ; Vikhlyantsev, O. ; Vilakazi, Zabulon ; Villalobos Baillie, Orlando ; Vinogradov, Alexander A. ; Vinogradov, Leonid ; Vinogradov, Yury I. ; Virgili, Tiziano ; Viyogi, Yogendra P. ; Vodopyanov, Alexander ; Voloshin, Kirill ; Voloshin, Sergei ; Volpe, Giacomo ; Haller, Barthélémy von ; Vranić, Danilo ; Vrláková, Janka ; Vulpescu, Bogdan ; Wagner, Boris ; Wagner, V. ; Wan, R. ; Wang, D. ; Wang, Y. ; Wang, Y. ; Watanabe, K. ; Wessels, Johannes P. ; Westerhoff, Uwe ; Wiechula, Jens ; Wikne, Jon ; Wilde, Martin ; Wilk, A. ; Wilk, Grzegorz Andrzej ; Williams, M. Crispin S. ; Windelband, Bernd ; Yang, H. ; Yasnopolskiy, S. ; Yi, J. ; Yin, Zhongbao ; Yokoyama, Hiroki ; Yoo, In-Kwon ; Yuan, X. ; Yushmanov, Igor E. ; Zabrodin, E. ; Zampolli, Chiara ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zbroszczyk, Hanna Paulina ; Zelnicek, P. ; Zenin, A. ; Zgura, I. ; Zhalov, Mikhail ; Zhang, X. ; Zhou, D. ; Zhu, X. ; Zichichi, Antonino ; Zinovjev, Gennady M. ; Zoccarato, Y. ; Zynovyev, M.
The first measurement of two-pion Bose–Einstein correlations in central Pb–Pb collisions at √sNN=2.76 TeV at the Large Hadron Collider is presented. We observe a growing trend with energy now not only for the longitudinal and the outward but also for the sideward pion source radius. The pion homogeneity volume and the decoupling time are significantly larger than those measured at RHIC.
Aamodt, Kenneth ; Abrahantes Quintana, A. ; Adamová, Dagmar ; Adare, A.M. ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agocs, A.G. ; Agostinelli, A. ; Aguilar Salazar, S. ; Ahammed, Zubayer ; Ahmad, Nazeer ; Ahmad Masoodi, A. ; Ahn, Sang Un ; Akindinov, Alexander ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alfaro Molina, Jose Ruben ; Alici, Andrea ; Alkin, Anton ; Almaráz Aviña, E. ; Alme, Johan ; Alt, Torsten ; Altini, V. ; Altsybeev, Igor ; Andrei, Cristian ; Andronic, Anton ; Anguelov, Venelin ; Anson, Christopher Daniel ; Antičić, Tome ; Antinori, Federico ; Antonioli, Pietro ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arbor, N. ; Arcelli, Silvia ; Arend, A. ; Armesto, Néstor ; Arnaldi, Roberta ; Aronsson, Tomas Robert ; Arsene, Ionut Cristian ; Asryan, A. ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, T.C. ; Äystö, J. ; Azmi, Mohd Danish ; Bach, Matthias ; Badalà, Angela ; Baek, Yong Wook ; Bailhache, Raphaëlle ; Bala, Remu ; Baldini Ferroli, Rinaldo ; Baldisseri, Alberto ; Baldit, A. ; Bán, J. ; Barbera, Roberto ; Barile, Francesco ; Barnaföldi, Gergely Gábor ; Barnby, Lee Stuart ; Barret, Valerie ; Bartke, Jerzy ; Basile, Maurizio ; Bastid, Nicole ; Bathen, Bastian ; Batigne, Guillaume ; Batyunya, Boris ; Baumann, C. ; Bearden, Ian Gardner ; Beck, Hans ; Belikov, Iouri ; Bellini, Francesca ; Bellwied, Rene ; Belmont-Moreno, Ernesto ; Beolè, Stefania ; Berceanu, Ionela ; Bercuci, Alexandru ; Berdermann, E. ; Berdnikov, Yaroslav ; Bergmann, C. ; Betev, Latchezar ; Bhasin, Anju ; Bhati, Ashok Kumar ; Bianchi, Livio ; Bianchi, Nicola ; Bianchin, Chiara ; Bielčík, Jaroslav ; Bielčíková, Jana ; Bilandzic, Ante ; Biolcati, E. ; Blanc, A. ; Blanco, Fernando ; Blanco, Fernando ; Blau, Dmitry S. ; Blume, Christoph ; Bock, N. ; Bogdanov, Alexey A. ; Bøggild, Hans ; Bogolyubsky, M. ; Boldizsár, László ; Bombara, Marek ; Bombonati, C. ; Book, Julian ; Borel, Hervé ; Borissov, Alexander ; Bortolin, C. ; Bose, S. ; Bossú, Francesco ; Botje, Michiel ; Böttger, Stefan ; Boyer, B. ; Braun-Munzinger, Peter ; Bravina, L. ; Bregant, Marco ; Breitner, Timo ; Broz, Michal ; Brun, René ; Bruna, Elena ; Bruno, Giuseppe Eugenio ; Budnikov, Dmitry ; Büsching, Henner ; Bufalino, Stefania ; Busch, Oliver ; Buthelezi, Edith Zinhle ; Caffarri, Davide ; Cai, Xiao ; Caines, Helen Louise ; Calvo Villar, Ernesto ; Camerini, Paolo ; Canoa Roman, Veronica ; Cara Romeo, G. ; Carena, Francesco ; Carena, Wisla ; Carminati, F. ; Casanova Díaz, A. ; Caselle, M. ; Castillo Castellanos, Javier Ernesto ; Catanescu, V. ; Cavicchioli, Costanza ; Čepila, Jan ; Cerello, Piergiorgio ; Chang, B. ; Chapeland, Sylvain ; Charvet, Jean-Luc Fernand ; Chattopadhyay, S. ; Chattopadhyay, S. ; Cherney, Michael Gerard ; Cheshkov, Cvetan Valeriev ; Cheynis, Brigitte ; Chiavassa, E. ; Chibante Barroso, Vasco Miguel ; Chinellato, David Dobrigkeit ; Chochula, Peter ; Chojnacki, Marek ; Christakoglou, Panagiotis ; Christensen, Christian Holm ; Christiansen, Peter L. ; Chujo, Tatsuya ; Cicalò, Corrado ; Cifarelli, Luisa ; Cindolo, Federico ; Cleymans, Jean Willy Andre ; Coccetti, F. ; Coffin, J.-P. ; Conesa Balbastre, Gustavo ; Conesa del Valle, Zaida ; Constantin, P. ; Contin, Giacomo ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortés Maldonado, Ismael ; Cortese, Pietro ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Cotallo, M.E. ; Crescio, E. ; Crochet, Philippe ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; D Erasmo, G. ; Dainese, Andrea ; Dalsgaard, H.H. ; Danu, Andrea ; Das, Debasish ; Das, Indranil ; Dash, Ajay Kumar ; Dash, Sadhana ; De, Sudipan ; De Azevedo Moregula, A. ; de Barros, G.O.V. ; De Caro, Annalisa ; De Cataldo, Giacinto ; Cuveland, Jan de ; De Falco, Alessandro ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; de Rooij, R. ; Del Castillo Sanchez, E. ; Delagrange, H. ; Delgado Mercado, Y. ; Dellacasa, G. ; Deloff, Andrzej ; Demanov, V. ; Dénes, Ervin Sandor ; Deppman, A. ; Di Bari, Domenico ; Di Giglio, C. ; Di Liberto, S. ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Dietel, Thomas ; Divià, Roberto ; Djuvsland, Øystein ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Domínguez, I. ; Dönigus, Benjamin ; Dordic, Olja ; Driga, O. ; Dubey, Anand Kumar ; Ducroux, Laurent ; Dupieux, Pascal ; Dutta Majumdar, A.K. ; Dutta Majumdar, M.R. ; Elia, Domenico ; Emschermann, D. ; Engel, Heiko ; Erdal, H.A. ; Espagnon, Bruno ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evrard, S. ; Eyyubova, Gyulnara ; Fabris, Daniela ; Faivre, Julien ; Falchieri, D. ; Fantoni, Alessandra ; Fasel, Markus ; Fearick, R. ; Fedunov, A. ; Fehlker, D. ; Fekete, V. ; Felea, Daniel ; Feofilov, Grigori A. ; Fernández Téllez, Arturo ; Gonzalez Ferreiro, Elena ; Ferretti, Alessandro ; Ferretti, R. ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Fini, R. ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Fragkiadakis, M. ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furano, F. ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhøje, Jens Jørgen ; Gadrat, S. ; Gagliardi, Martino ; Gago, A. ; Gallio, Mauro ; Ganoti, Paraskevi ; Garabatos, Chilo ; Garcia-Solis, Edmundo Javier ; Gemme, R. ; Gerhard, J. ; Germain, Marie ; Geuna, C. ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, B. ; Ghosh, Premomoy ; Gianotti, Paola ; Girard, M.R. ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glässel, Peter ; Gomez, R. ; González Trueba, Laura Helena ; González Zamora, Pedro ; Gorbunov, Sergey ; Gotovac, Sven ; Grabski, Varlen ; Graczykowski, Łukasz Kamil ; Grajcarek, R. ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoriev, Vladislav A. ; Grigoryan, Ara ; Grigoryan, Smbat ; Grinyov, Boris V. ; Grion, Nevio ; Gros, P. ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Guber, Fedor ; Guernane, Rachid ; Guerra Gutierrez, C. ; Guerzoni, Barbara ; Gulbrandsen, Kristjan Herlache ; Gulkanyan, Hrant ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Gutbrod, H. ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Hanratty, Luke David ; Harmanova, Z. ; Harris, John W. ; Hartig, M. ; Hasegan, D. ; Hatzifotiadou, Despina ; Hayrapetyan, A. ; Heide, Markus ; Heinz, Mark Thomas ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Herrera Corral, Gerardo Antonio ; Herrmann, Norbert ; Hetland, Kristin Fanebust ; Hicks, B. ; Hille, P.T. ; Hippolyte, Boris ; Horaguchi, T. ; Hori, Y. ; Hristov, Peter ; Hřivnáčová, I. ; Huang, M. ; Huber, S. ; Humanic, Thomas J. ; Hwang, Dae Sung ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Incani, E. ; Innocenti, Gian Michele ; Ippolitov, Mikhail ; Irfan, M. ; Ivan, C. ; Ivanov, A. ; Ivanov, Marian ; Ivanov, V. ; Jacholkowski, Adam Wlodzimierz ; Jacobs, Peter Martin ; Jancurová, L. ; Jangal, S. ; Janik, Malgorzata Anna ; Janik, R. ; Jayarathna, Pahula Hewage Sandun Yasassri ; Jena, Satyajit ; Jirden, L. ; Jones, Goronwy Tudor ; Jones, Peter Graham ; Jovanović, P. ; Jung, H. ; Jung, W. ; Jusko, Anton ; Kalcher, S. ; Kaliňák, Peter ; Kalisky, M. ; Kalliokoski, T. ; Kalweit, Alexander Philipp ; Kamermans, R. ; Kanaki, K. ; Kang, E. ; Kang, Ju Hwan ; Kaplin, Vladimir ; Karasu Uysal, Ayben ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kazantsev, Andrey ; Kebschull, Udo ; Keidel, Ralf ; Khan, M.M. ; Khan, P. ; Khanzadeev, Alexei ; Kharlov, Yury ; Kileng, Bjarte ; Kim, D.J. ; Kim, D.S. ; Kim, D.W. ; Kim, J.H. ; Kim, J.S. ; Kim, M. ; Kim, S. ; Kim, S.H. ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kliemant, Michael ; Kluge, Alexander ; Knichel, Michael Linus ; Koch, K. ; Köhler, Markus Konrad ; Kolojvari, Anatoly ; Kondratiev, Valery P. ; Kondratyeva, Natalia ; Konevskih, A. ; Kornaś, Ewelina ; Kottachchi Kankanamge Don, C. ; Kour, R. ; Kowalski, Marek ; Kox, Serge ; Koyithatta Meethaleveedu, Greeshma ; Kozlov, K. ; Kral, Jiří ; Králik, Ivan ; Kramer, F. ; Kraus, Ingrid ; Krawutschke, T. ; Kretz, Matthias ; Krivda, Marian ; Krizek, Filip ; Krus, M. ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucheriaev, Yury ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, Alexey B. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kushpil, V. ; Kweon, Min Jung ; Kwon, Youngil ; La Rocca, Paola ; Ladron de Guevara, Pedro ; Lafage, V. ; Lakomov, Igor ; Lara Martinez, Camilo Ernesto ; Larsen, D.T. ; Lazzeroni, C. ; Le Bornec, Y. ; Lea, Ramona ; Lechman, M. ; Lee, K.S. ; Lee, S.C. ; Lefèvre, F. ; Lehnert, Jörg ; Leistam, L. ; Lenhardt, M. ; Lenti, Vito ; León Monzón, Ildefonso ; León Vargas, H. ; Lévai, Péter ; Li, X. ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Liu, L. ; Loggins, Vera Renee ; Loginov, Vitaly ; Lohn, S. ; Lohner, D. ; Loizides, Constantinos ; Loo, K.K. ; Lopez, Xavier Bernard ; López Noriega, M. ; López Torres, Ernesto ; Løvhøiden, G. ; Lu, X.-G. ; Lüttig, Philipp ; Lunardon, Marcello ; Luparello, Grazia ; Luquin, L. ; Luzzi, C. ; Ma, K. ; Ma, R. ; Madagodahettige-Don, D.M. ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, Durga Prasad ; Maire, Antonin ; Malaev, Mikhail ; Maldonado Cervantes, Ivonne Alicia ; MalʼKevich, D. ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Mao, Yaxian ; Marchisone, Massimiliano ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marín, Ana ; Markert, Christina ; Martashvili, Irakli ; Martinengo, Paolo ; Martínez Hernández, Mario Iván ; Martínez Davalos, A. ; Martínez Garcia, Ginés ; Martynov, Yevgen ; Mas, Alexis Jean-Michel ; Masciocchi, Silvia ; Masera, Massimo ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastromarco, Mario ; Mastroserio, Annalisa ; Matthews, Z.L. ; Matyja, Adam Tomasz ; Mayani, D. ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mendez Lorenzo, P. ; Mercado Pérez, Jorge ; Meres, Michal ; Miake, Yasuo ; Midori, J. ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Miśkowiec, Dariusz Czesław ; Mitu, C. ; Mlynarz, J. ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Monteno, M. ; Montes Prado, Esther ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Müller, H. ; Muhuri, Sanjib ; Munhoz, Marcelo Gameiro ; Musa, Luciano ; Musso, A. ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Navach, F. ; Navin, S. ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nazarov, G. ; Nedosekin, Alexander ; Nendaz, F. ; Nicassio, Maria ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikolic, V. ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, B.S. ; Nilsson, M.S. ; Noferini, Francesco ; Nooren, Gerardus ; Novitzky, Norbert ; Nyanin, Alexander ; Nyatha, A. ; Nygaard, C. ; Nystrand, Joakim Ingemar ; Obayashi, H. ; Ochirov, A. ; Oeschler, Helmut ; Oh, Sun Kun ; Oleniacz, Janusz ; Oppedisano, Chiara ; Ortiz Velasquez, Antonio ; Ortona, G. ; Oskarsson, Anders Nils Erik ; Ostrowski, P. ; Otterlund, I. ; Otwinowski, Jacek Tomasz ; Øvrebekk, G. ; Oyama, Ken ; Ozawa, K. ; Pachmayer, Yvonne C. ; Pachr, Miloš ; Padilla, F. ; Pagano, Paola ; Paić, Guy ; Painke, F. ; Pajares Vales, Carlos ; Pal, S. ; Pal, Susanta Kumar ; Palaha, A. ; Palmeri, A. ; Pappalardo, Giuseppe Salvatore ; Park, WooJin ; Paticchio, Vincenzo ; Pavlinov, A. ; Pawlak, Tomasz Jan ; Peitzmann, Thomas ; Peresunko, Dmitry Yurevich ; Pérez Lara, Carlos Eugenio ; Perini, D. ; Perrino, D. ; Peryt, Wiktor Stanislaw ; Pesci, A. ; Peskov, Vladimir ; Pestov, Yury N. ; Peters, A.J. ; Petráček, Vojtech ; Petran, M. ; Petris, M. ; Petrov, P. ; Petrovici, Mihai A. ; Petta, Catia ; Piano, Stefano ; Piccotti, A. ; Pikna, Miroslav ; Pillot, Philippe ; Pinazza, Ombretta ; Pinsky, Lawrence ; Pitz, N. ; Piuz, F. ; Piyarathna, Danthasinghe B. ; Platt, R. ; 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Rohr, David ; Röhrich, Dieter ; Romita, Rosa ; Ronchetti, Federico ; Rosinský, P. ; Rosnet, Philippe ; Rossegger, S. ; Rossi, Andrea ; Roukoutakis, Filimon ; Rousseau, S. ; Roy, Christelle Sophie ; Roy, Pradip Kumar ; Rubio Montero, Antonio Juan ; Rui, Rinaldo ; Ryabinkin, Evgeny ; Rybicki, Andrzej ; Sadovskiy, Sergey ; Šafařík, Karel ; Sahoo, Raghunath ; Sahu, Pradip Kumar ; Saiz, P. ; Sakai, Shingo ; Sakata, D. ; Salgado, Carlos A. ; Sambyal, Sanjeev Singh ; Samsonov, Vladimir ; Šándor, Ladislav ; Sandoval, Andres ; Sano, Masato ; Sano, S. ; Santo, R. ; Santoro, R. ; Sarkamo, J. ; Saturnini, P. ; Scapparone, Eugenio ; Scarlassara, Fernando ; Scharenberg, Rolf Paul ; Schiaua, Claudiu Cornel ; Schicker, Rainer ; Schmidt, Christian Joachim ; Schmidt, Hans Rudolf ; Schreiner, S. ; Schuchmann, Simone ; Schukraft, Jürgen ; Schutz, Yves Roland ; Schwarz, Kilian ; Schweda, Kai ; Scioli, Gilda ; Scomparin, Enrico ; Scott, P.A. ; Scott, Rebecca Michelle ; Segato, G. ; Senyukov, Serhiy ; Seo, Jeewon ; 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Crispin S. ; Windelband, Bernd ; Yang, H. ; Yasnopolskiy, S. ; Yi, J. ; Yin, Zhongbao ; Yokoyama, Hiroki ; Yoo, In-Kwon ; Yuan, X. ; Yushmanov, Igor E. ; Zabrodin, E. ; Zach, C. ; Zampolli, Chiara ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zaviyalov, Nikolaj ; Zbroszczyk, Hanna Paulina ; Zelnicek, P. ; Zenin, A. ; Zgura, I. ; Zhalov, Mikhail ; Zhang, X. ; Zhou, D. ; Zhou, F. ; Zhou, Y. ; Zhu, X. ; Zichichi, Antonino ; Zinovjev, Gennady M. ; Zoccarato, Y. ; Zynovyev, M.
Rapidity and transverse momentum dependence of inclusive J/ψ production in pp collisions at √s=7 TeV
(2011)
Aamodt, Kenneth ; Abrahantes Quintana, A. ; Adamová, Dagmar ; Adare, A.M. ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agocs, A.G. ; Agostinelli, A. ; Aguilar Salazar, S. ; Ahammed, Zubayer ; Ahmad, Nazeer ; Ahmad Masoodi, A. ; Ahn, Sang Un ; Akindinov, Alexander ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alfaro Molina, Jose Ruben ; Alici, Andrea ; Alkin, Anton ; Almaráz Aviña, E. ; Alme, Johan ; Alt, Torsten ; Altini, V. ; Altsybeev, Igor ; Andrei, Cristian ; Andronic, Anton ; Anguelov, Venelin ; Anson, Christopher Daniel ; Antičić, Tome ; Antinori, Federico ; Antonioli, Pietro ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arbor, N. ; Arcelli, Silvia ; Arend, A. ; Armesto, Néstor ; Arnaldi, Roberta ; Aronsson, Tomas Robert ; Arsene, Ionut Cristian ; Asryan, A. ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, T.C. ; Äystö, J. ; Azmi, Mohd Danish ; Bach, Matthias ; Badalà, Angela ; Baek, Yong Wook ; Bailhache, Raphaëlle ; Bala, Remu ; Baldini Ferroli, Rinaldo ; Baldisseri, Alberto ; Baldit, A. ; Bán, J. ; Barbera, Roberto ; Barile, Francesco ; Barnaföldi, Gergely Gábor ; Barnby, Lee Stuart ; Barret, Valerie ; Bartke, Jerzy ; Basile, Maurizio ; Bastid, Nicole ; Bathen, Bastian ; Batigne, Guillaume ; Batyunya, Boris ; Baumann, C. ; Bearden, Ian Gardner ; Beck, Hans ; Belikov, Iouri ; Bellini, Francesca ; Bellwied, Rene ; Belmont-Moreno, Ernesto ; Beolè, Stefania ; Berceanu, Ionela ; Bercuci, Alexandru ; Berdermann, E. ; Berdnikov, Yaroslav ; Bergmann, C. ; Betev, Latchezar ; Bhasin, Anju ; Bhati, Ashok Kumar ; Bianchi, Livio ; Bianchi, Nicola ; Bianchin, Chiara ; Bielčík, Jaroslav ; Bielčíková, Jana ; Bilandzic, Ante ; Biolcati, E. ; Blanc, A. ; Blanco, Fernando ; Blanco, Fernando ; Blau, Dmitry S. ; Blume, Christoph ; Bock, N. ; Bogdanov, Alexey A. ; Bøggild, Hans ; Bogolyubsky, M. ; Boldizsár, László ; Bombara, Marek ; Bombonati, C. ; Book, Julian ; Borel, Hervé ; Borissov, Alexander ; Bortolin, C. ; Bose, S. ; Bossú, Francesco ; Botje, Michiel ; Böttger, Stefan ; Boyer, B. ; Braun-Munzinger, Peter ; Bravina, L. ; Bregant, Marco ; Breitner, Timo ; Broz, Michal ; Brun, René ; Bruna, Elena ; Bruno, Giuseppe Eugenio ; Budnikov, Dmitry ; Büsching, Henner ; Bufalino, Stefania ; Busch, Oliver ; Buthelezi, Edith Zinhle ; Caffarri, Davide ; Cai, Xiao ; Caines, Helen Louise ; Calvo Villar, Ernesto ; Camerini, Paolo ; Canoa Roman, Veronica ; Cara Romeo, G. ; Carena, Francesco ; Carena, Wisla ; Carminati, F. ; Casanova Díaz, A. ; Caselle, M. ; Castillo Castellanos, Javier Ernesto ; Catanescu, V. ; Cavicchioli, Costanza ; Čepila, Jan ; Cerello, Piergiorgio ; Chang, B. ; Chapeland, Sylvain ; Charvet, Jean-Luc Fernand ; Chattopadhyay, S. ; Chattopadhyay, S. ; Cherney, Michael Gerard ; Cheshkov, Cvetan Valeriev ; Cheynis, Brigitte ; Chiavassa, E. ; Chibante Barroso, Vasco Miguel ; Chinellato, David Dobrigkeit ; Chochula, Peter ; Chojnacki, Marek ; Christakoglou, Panagiotis ; Christensen, Christian Holm ; Christiansen, Peter L. ; Chujo, Tatsuya ; Cicalò, Corrado ; Cifarelli, Luisa ; Cindolo, Federico ; Cleymans, Jean Willy Andre ; Coccetti, F. ; Coffin, J.-P. ; Conesa Balbastre, Gustavo ; Conesa del Valle, Zaida ; Constantin, P. ; Contin, Giacomo ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortés Maldonado, Ismael ; Cortese, Pietro ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Cotallo, M.E. ; Crescio, E. ; Crochet, Philippe ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; D Erasmo, G. ; Dainese, Andrea ; Dalsgaard, H.H. ; Danu, Andrea ; Das, Debasish ; Das, Indranil ; Dash, Ajay Kumar ; Dash, Sadhana ; De, Sudipan ; De Azevedo Moregula, A. ; de Barros, G.O.V. ; De Caro, Annalisa ; De Cataldo, Giacinto ; Cuveland, Jan de ; De Falco, Alessandro ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; de Rooij, R. ; Del Castillo Sanchez, E. ; Delagrange, H. ; Delgado Mercado, Y. ; Dellacasa, G. ; Deloff, Andrzej ; Demanov, V. ; Dénes, Ervin Sandor ; Deppman, A. ; Di Bari, Domenico ; Di Giglio, C. ; Di Liberto, S. ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Dietel, Thomas ; Divià, Roberto ; Djuvsland, Øystein ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Domínguez, I. ; Dönigus, Benjamin ; Dordic, Olja ; Driga, O. ; Dubey, Anand Kumar ; Ducroux, Laurent ; Dupieux, Pascal ; Dutta Majumdar, A.K. ; Dutta Majumdar, M.R. ; Elia, Domenico ; Emschermann, D. ; Engel, Heiko ; Erdal, H.A. ; Espagnon, Bruno ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evrard, S. ; Eyyubova, Gyulnara ; Fabris, Daniela ; Faivre, Julien ; Falchieri, D. ; Fantoni, Alessandra ; Fasel, Markus ; Fearick, R. ; Fedunov, A. ; Fehlker, D. ; Fekete, V. ; Felea, Daniel ; Feofilov, Grigori A. ; Fernández Téllez, Arturo ; Gonzalez Ferreiro, Elena ; Ferretti, Alessandro ; Ferretti, R. ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Fini, R. ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Fragkiadakis, M. ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furano, F. ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhøje, Jens Jørgen ; Gadrat, S. ; Gagliardi, Martino ; Gago, A. ; Gallio, Mauro ; Ganoti, Paraskevi ; Garabatos, Chilo ; Garcia-Solis, Edmundo Javier ; Gemme, R. ; Gerhard, J. ; Germain, Marie ; Geuna, C. ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, B. ; Ghosh, Premomoy ; Gianotti, Paola ; Girard, M.R. ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glässel, Peter ; Gomez, R. ; González Trueba, Laura Helena ; González Zamora, Pedro ; Gorbunov, Sergey ; Gotovac, Sven ; Grabski, Varlen ; Graczykowski, Łukasz Kamil ; Grajcarek, R. ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoriev, Vladislav A. ; Grigoryan, Ara ; Grigoryan, Smbat ; Grinyov, Boris V. ; Grion, Nevio ; Gros, P. ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Guber, Fedor ; Guernane, Rachid ; Guerra Gutierrez, C. ; Guerzoni, Barbara ; Gulbrandsen, Kristjan Herlache ; Gulkanyan, Hrant ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Gutbrod, H. ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Hanratty, Luke David ; Harmanova, Z. ; Harris, John W. ; Hartig, M. ; Hasegan, D. ; Hatzifotiadou, Despina ; Hayrapetyan, A. ; Heide, Markus ; Heinz, Mark Thomas ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Herrera Corral, Gerardo Antonio ; Herrmann, Norbert ; Hetland, Kristin Fanebust ; Hicks, B. ; Hille, P.T. ; Hippolyte, Boris ; Horaguchi, T. ; Hori, Y. ; Hristov, Peter ; Hřivnáčová, I. ; Huang, M. ; Huber, S. ; Humanic, Thomas J. ; Hwang, D.S. ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Incani, E. ; Innocenti, Gian Michele ; Ippolitov, Mikhail ; Irfan, M. ; Ivan, C. ; Ivanov, A. ; Ivanov, Marian ; Ivanov, V. ; Jacholkowski, Adam Wlodzimierz ; Jacobs, Peter Martin ; Jancurová, L. ; Jangal, S. ; Janik, Malgorzata Anna ; Janik, R. ; Jayarathna, Pahula Hewage Sandun Yasassri ; Jena, Satyajit ; Jirden, L. ; 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The ALICE experiment at the LHC has studied inclusive J/ψ production at central and forward rapidities in pp collisions at √s=7 TeV. In this Letter, we report on the first results obtained detecting the J/ψ through the dilepton decay into e+e− and μ+μ− pairs in the rapidity ranges |y|<0.9 and 2.5<y<4, respectively, and with acceptance down to zero pT. In the dielectron channel the analysis was carried out on a data sample corresponding to an integrated luminosity Lint=5.6 nb−1 and the number of signal events is NJ/ψ=352±32(stat.)±28(syst.); the corresponding figures in the dimuon channel are Lint=15.6 nb−1 and NJ/ψ=1924±77(stat.)±144(syst.). The measured production cross sections are σJ/ψ(|y|<0.9)=10.7±1.0(stat.)±1.6(syst.)−2.3+1.6(syst.pol.)μb and σJ/ψ(2.5<y<4)=6.31±0.25(stat.)±0.76(syst.)−1.96+0.95(syst.pol.)μb. The differential cross sections, in transverse momentum and rapidity, of the J/ψ were also measured.
Harmonic decomposition of two particle angular correlations in Pb–Pb collisions at √sNN=2.76 TeV
(2012)
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Ivanov, V. ; Ivanytskyi, O. ; Jacobs, Peter Martin ; Jancurová, L. ; Jangal, S. ; Janik, Malgorzata Anna ; Janik, R. ; Jayarathna, Pahula Hewage Sandun Yasassri ; Jena, Satyajit ; Jiménez Bustamante, Raúl Tonatiuh ; Jirden, L. ; Jones, Peter Graham ; Jung, H. ; Jung, W. ; Jusko, Anton ; Kalcher, S. ; Kaliňák, Peter ; Kalisky, M. ; Kalliokoski, T. ; Kalweit, Alexander Philipp ; Kanaki, K. ; Kang, Ju Hwan ; Kaplin, Vladimir ; Karasu Uysal, Ayben ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kazantsev, Andrey ; Kebschull, Udo ; Keidel, Ralf ; Khan, M.M. ; Khan, P. ; Khan, Shuaib Ahmad ; Khanzadeev, Alexei ; Kharlov, Yury ; Kileng, Bjarte ; Kim, B. ; Kim, D.J. ; Kim, D.W. ; Kim, J.H. ; Kim, J.S. ; Kim, M. ; Kim, S. ; Kim, S.H. ; Kim, T. ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kliemant, Michael ; Kluge, Alexander ; Knichel, Michael Linus ; Koch, K. ; Köhler, Markus Konrad ; Kolojvari, Anatoly ; Kondratiev, Valery P. ; Kondratyeva, Natalia ; Konevskikh, Artem ; Kottachchi Kankanamge Don, C. ; Kour, R. ; Kowalski, Marek ; Kox, Serge ; Koyithatta Meethaleveedu, Greeshma ; Kral, Jiří ; Králik, Ivan ; Kramer, F. ; Kraus, Ingrid ; Krawutschke, T. ; Kretz, Matthias ; Krivda, Marian ; Krizek, Filip ; Krus, M. ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucheriaev, Yury ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, Alexey B. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kushpil, V. ; Kweon, Min Jung ; Kwon, Youngil ; La Rocca, Paola ; Ladron de Guevara, Pedro ; Lakomov, Igor ; Lara Martinez, Camilo Ernesto ; Lardeux, Antoine Xavier ; Larsen, D.T. ; Lazzeroni, C. ; Le Bornec, Y. ; Lea, Ramona ; Lechman, M. ; Lee, K.S. ; Lee, S.C. ; Lefèvre, F. ; Lehnert, Jörg ; Leistam, L. ; Lenhardt, M. ; Lenti, Vito ; León Monzón, Ildefonso ; León Vargas, H. ; Lévai, Péter ; Li, X. ; Lien, Jørgen André ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Liu, L. ; Lønne, Per-Ivar ; Loggins, Vera Renee ; Loginov, Vitaly ; Lohn, S. ; Lohner, D. ; Loizides, Constantinos ; Loo, K.K. ; Lopez, Xavier Bernard ; López Torres, Ernesto ; Løvhøiden, G. ; Lu, X.-G. ; Lüttig, Philipp ; Lunardon, Marcello ; Luo, J. ; Luparello, Grazia ; Luquin, L. ; Luzzi, C. ; Ma, R. ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, Durga Prasad ; Maire, Antonin ; Malaev, Mikhail ; Maldonado Cervantes, Ivonne Alicia ; Malinina, Liudmila ; MalʼKevich, D. ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Mao, Yaxian ; Marchisone, Massimiliano ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marín, Ana ; Markert, Christina ; Martashvili, Irakli ; Martinengo, Paolo ; Martínez Hernández, Mario Iván ; Martínez Davalos, A. ; Martínez Garcia, Ginés ; Martynov, Yevgen ; Mas, Alexis Jean-Michel ; Masciocchi, Silvia ; Masera, Massimo ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastromarco, Mario ; Mastroserio, Annalisa ; Matthews, Z.L. ; Matyja, Adam Tomasz ; Mayani, D. ; Mayer, Christoph ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mercado Pérez, Jorge ; Meres, Michal ; Miake, Yasuo ; Michalon, A. ; Midori, J. ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Mishra, Aditya Nath ; Miśkowiec, Dariusz Czesław ; Mitu, C. ; Mlynarz, J. ; Mohanty, A.K. ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Monteno, M. ; Montes Prado, Esther ; Moon, T. ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Müller, H. ; Muhuri, Sanjib ; Munhoz, Marcelo Gameiro ; Musa, Luciano ; Musso, A. ; Nagle, J.L. ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Naumov, N.P. ; Navin, S. ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nazarov, G. ; Nedosekin, Alexander ; Nicassio, Maria ; Nielsen, Borge Svane ; Niida, Takafumi ; Nikolaev, Sergey ; Nikolic, V. ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, B.S. ; Nilsson, M.S. ; Noferini, Francesco ; Nomokonov, Petr V. ; Nooren, Gerardus ; Novitzky, Norbert ; Nyanin, Alexander ; Nyatha, A. ; Nygaard, C. ; Nystrand, Joakim Ingemar ; Obayashi, H. ; Ochirov, A. ; Oeschler, Helmut ; Oh, Sun Kun ; Oleniacz, Janusz ; Oppedisano, Chiara ; Ortiz Velasquez, Antonio ; Ortona, G. ; Oskarsson, Anders Nils Erik ; Otterlund, I. ; Otwinowski, Jacek Tomasz ; Øvrebekk, G. ; Oyama, Ken ; Pachmayer, Yvonne C. ; Pachr, Miloš ; Padilla, F. ; Pagano, Paola ; Paić, Guy ; Painke, F. ; Pajares Vales, Carlos ; Pal, S. ; Pal, Susanta Kumar ; Palaha, A. ; Palmeri, A. ; Pappalardo, Giuseppe Salvatore ; Park, WooJin ; Passfeld, Annika ; Patalakha, D.I. ; Paticchio, Vincenzo ; Pavlinov, A. ; Pawlak, Tomasz Jan ; Peitzmann, Thomas ; Filho, Elienos Pereira de Oliveira ; Peresunko, Dmitry Yurevich ; Pérez Lara, Carlos Eugenio ; Pérez Lezama, Edgar ; Perini, D. ; 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Wessels, Johannes P. ; Westerhoff, Uwe ; Wiechula, Jens ; Wikne, Jon ; Wilde, Martin ; Wilk, A. ; Wilk, Grzegorz Andrzej ; Williams, M. Crispin S. ; Windelband, Bernd ; Xaplanteris Karampatsos, L. ; Yang, H. ; Yasnopolskiy, S. ; Yi, J. ; Yin, Zhongbao ; Yokoyama, Hiroki ; Yoo, In-Kwon ; Yoon, J. ; Yu, W. ; Yuan, X. ; Yushmanov, Igor E. ; Zach, C. ; Zampolli, Chiara ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zaviyalov, Nikolaj ; Zbroszczyk, Hanna Paulina ; Zelnicek, P. ; Zgura, I. ; Zhalov, Mikhail ; Zhang, X. ; Zhou, D. ; Zhou, F. ; Zhou, Y. ; Zhu, X. ; Zichichi, Antonino ; Zimmermann, Alice ; Zinovjev, Gennady M. ; Zoccarato, Y. ; Zynovyev, M.
Angular correlations between unidentified charged trigger (t) and associated (a) particles are measured by the ALICE experiment in Pb–Pb collisions at √sNN=2.76 TeV for transverse momenta 0.25<pTt,a<15 GeV/c, where pTt>pTa. The shapes of the pair correlation distributions are studied in a variety of collision centrality classes between 0 and 50% of the total hadronic cross section for particles in the pseudorapidity interval |η|<1.0. Distributions in relative azimuth Δϕ≡ϕt−ϕa are analyzed for |Δη|≡|ηt−ηa|>0.8, and are referred to as “long-range correlations”. Fourier components VnΔ≡〈cos(nΔϕ)〉 are extracted from the long-range azimuthal correlation functions. If particle pairs are correlated to one another through their individual correlation to a common symmetry plane, then the pair anisotropy VnΔ(pTt,pTa) is fully described in terms of single-particle anisotropies vn(pT) as VnΔ(pTt,pTa)=vn(pTt)vn(pTa). This expectation is tested for 1⩽n⩽5 by applying a global fit of all VnΔ(pTt,pTa) to obtain the best values vn{GF}(pT). It is found that for 2⩽n⩽5, the fit agrees well with data up to pTa∼3–4 GeV/c, with a trend of increasing deviation as pTt and pTa are increased or as collisions become more peripheral. This suggests that no pair correlation harmonic can be described over the full 0.25<pT<15 GeV/c range using a single vn(pT) curve; such a description is however approximately possible for 2⩽n⩽5 when pTa<4 GeV/c. For the n=1 harmonic, however, a single v1(pT) curve is not obtained even within the reduced range pTa<4 GeV/c.
Aamodt, Kenneth ; Abel, N. ; Abeysekara, U. ; Abrahantes Quintana, A. ; Abramyan, A. ; Adamová, Dagmar ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agocs, A.G. ; Aguilar Salazar, S. ; Ahammed, Zubayer ; Ahmad, A. ; Ahmad, Nazeer ; Ahn, Sang Un ; Akimoto, R. ; Akindinov, Alexander ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alfaro Molina, Jose Ruben ; Alici, Andrea ; Almaráz Aviña, E. ; Alme, Johan ; Alt, Torsten ; Altini, V. ; Altinpinar, Sedat ; Andrei, Cristian ; Andronic, Anton ; Anelli, G. ; Angelov, V. ; Anson, Christopher Daniel ; Antičić, Tome ; Antinori, Federico ; Antinori, S. ; Antipin, K. ; Antończyk, Dariusz ; Antonioli, Pietro ; Anzo, A. ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arcelli, Silvia ; Arceo, R. ; Arend, A. ; Armesto, Néstor ; Arnaldi, Roberta ; Aronsson, Tomas Robert ; Arsene, Ionut Cristian ; Asryan, A. ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, T.C. ; Äystö, J. ; Azmi, Mohd Danish ; Bablok, Sebastian ; Bach, Matthias ; Badalà, Angela ; 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De Gaspari, M. ; de Groot, J. ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; De Remigis, R. ; de Rooij, R. ; de Vaux, G. ; Delagrange, H. ; Delgado, Y. ; Dellacasa, G. ; Deloff, Andrzej ; Demanov, V. ; Dénes, Ervin Sandor ; Deppman, A. ; D’Erasmo, Ginevra ; Derkach, D. ; Devaux, A. ; Di Bari, Domenico ; Di Giglio, C. ; Di Liberto, S. ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Dialinas, M. ; Díaz, L. ; Díaz, R. ; Dietel, Thomas ; Divià, Roberto ; Djuvsland, Øystein ; Dobretsov, V. ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Dönigus, Benjamin ; Domínguez, I. ; Don, D.M.M. ; Dordic, Olja ; Dubey, Anand Kumar ; Dubuisson, J. ; Ducroux, Laurent ; Dupieux, Pascal ; Dutta Majumdar, A.K. ; Dutta Majumdar, M.R. ; Elia, Domenico ; Emschermann, D. ; Enokizono, A. ; Espagnon, Bruno ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evrard, S. ; Eyyubova, Gyulnara ; Fabjan, C.W. ; Fabris, Daniela ; Faivre, Julien ; Falchieri, D. ; Fantoni, Alessandra ; Fasel, Markus ; Fateev, O. ; Fearick, R. ; Fedunov, A. ; Fehlker, D. ; Fekete, V. ; Felea, Daniel ; Fenton-Olsen, B. ; Feofilov, Grigori A. ; Fernández Téllez, Arturo ; Gonzalez Ferreiro, Elena ; Ferretti, Alessandro ; Ferretti, R. ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Fini, R. ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floris, Michele ; Fodor, Zoltán ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Formenti, F. ; Fragiacomo, Enrico ; Fragkiadakis, M. ; Frankenfeld, Ulrich ; Frolov, A. ; Fuchs, Ulrich ; Furano, F. ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhøje, Jens Jørgen ; Gadrat, S. ; Gagliardi, Martino ; Gago, A. ; Gallio, Mauro ; Ganoti, Paraskevi ; Ganti, Murthy S. ; Garabatos, Chilo ; García Trapaga, C. ; Gebelein, J. ; Gemme, R. ; Germain, Marie ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, B. ; Ghosh, Premomoy ; Giraudo, G. ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glasow, R. ; Glässel, Peter ; Glenn, A. ; Gómez Jiménez, R. ; González Santos, H. ; González Trueba, Laura Helena ; González Zamora, Pedro ; Gorbunov, Sergey ; Gorbunov, Y. ; Gotovac, Sven ; Gottschlag, H. ; Grabski, Varlen ; Grajcarek, R. ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoriev, Vladislav A. ; Grigoryan, Ara ; Grigoryan, Smbat ; Grinyov, Boris V. ; Grion, Nevio ; Gros, P. ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Grosso, Raffaele ; Guber, Fedor ; Guernane, Rachid ; Guerra, C. ; Guerzoni, Barbara ; Gulbrandsen, Kristjan Herlache ; Gulkanyan, Hrant ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Gustafsson, H.-A. ; Gutbrod, H. ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Hamblen, J. ; Han, B.H. ; Harris, John W. ; Hartig, M. ; Harutyunyan, A. ; Hasch, D. ; Hasegan, D. ; Hatzifotiadou, Despina ; Hayrapetyan, A. ; Heide, Markus ; Heinz, Mark Thomas ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Hernández, C. ; Herrera Corral, Gerardo Antonio ; Herrmann, Norbert ; Hetland, Kristin Fanebust ; Hicks, B. ; Hiei, A. ; Hille, P.T. ; Hippolyte, Boris ; Horaguchi, T. ; Hori, Y. ; Hristov, Peter ; Hřivnáčová, I. ; Hu, S. ; Huang, M. ; Huber, S. ; Humanic, Thomas J. ; Hutter, Dirk ; Hwang, D.S. ; Ichou, R. ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Innocenti, P.G. ; Ippolitov, Mikhail ; Irfan, M. ; Ivan, C. ; Ivanov, A. ; Ivanov, Marian ; Ivanov, V. ; Iwasaki, T. ; Jacholkowski, Adam Wlodzimierz ; Jacobs, P. ; Jančurová, L. ; Jangal, S. ; Janik, R. ; Jena, Chitrasen ; Jena, Satyajit ; Jirden, L. ; Jones, Goronwy Tudor ; Jones, Peter Graham ; Jovanović, P. ; Jung, H. ; Jung, W. ; Jusko, Anton ; Kaidalov, A.B. ; Kalcher, S. ; Kaliňák, Peter ; Kalisky, M. ; Kalliokoski, T. ; Kalweit, Alexander Philipp ; Kamal, A. ; Kamermans, R. ; Kanaki, K. ; Kang, E. ; Kang, Ju Hwan ; Kapitan, J. ; Kaplin, Vladimir ; Kapusta, S. ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kazantsev, Andrey ; Kebschull, Udo ; Keidel, Ralf ; Khan, M.M. ; Khan, Shuaib Ahmad ; Khanzadeev, Alexei ; Kharlov, Yury ; Kikola, D. ; Kileng, Bjarte ; Kim, D.J. ; Kim, D.S. ; Kim, D.W. ; Kim, H.N. ; Kim, J. ; Kim, J.H. ; Kim, J.S. ; Kim, M. ; Kim, M. ; Kim, S.H. ; Kim, S. ; Kim, Y. ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kliemant, Michael ; Klovning, A. ; Kluge, Alexander ; Knichel, Michael Linus ; Kniege, Stefan ; Koch, K. ; Kolevatov, R. ; Kolojvari, Anatoly ; Kondratiev, Valery P. ; Kondratyeva, Natalia ; Konevskih, A. ; Kornaś, Ewelina ; Kour, R. ; Kowalski, Marek ; Kox, Serge ; Kozlov, K. ; Kral, Jiří ; Králik, Ivan ; Kramer, F. ; Kraus, Ingrid ; Kravčáková, Adela ; Krawutschke, T. ; Krivda, Marian ; Krumbhorn, D. ; Krus, M. ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucheriaev, Yury ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kumar, Lokesh ; Kumar, N. ; Kupczak, R. ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, A.N. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kushpil, V. ; Kutouski, M. ; Kvaerno, H. ; Kweon, Min Jung ; Kwon, Youngil ; La Rocca, Paola ; Lackner, F. ; Ladron de Guevara, Pedro ; Lafage, V. ; Lal, C. ; Lara Martinez, Camilo Ernesto ; Larsen, D.T. ; Laurenti, G. ; Lazzeroni, C. ; Le Bornec, Y. ; Le Bris, N. ; Lee, H. ; Lee, K.S. ; Lee, S.C. ; Lefèvre, F. ; Lenhardt, M. ; Leistam, L. ; Lehnert, Jörg ; Lenti, Vito ; León, H. ; León Monzón, Ildefonso ; León Vargas, H. ; Lévai, Péter ; Li, X. ; Li, Y. ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Liu, L. ; Loginov, Vitaly ; Lohn, S. ; Lopez, Xavier Bernard ; López Noriega, M. ; López-Ramírez, R. ; López Torres, Ernesto ; Løvhøiden, G. ; Lozea Feijo Soares, A. ; Lu, S. ; Lüttig, Philipp ; Lunardon, Marcello ; Luparello, Grazia ; Luquin, L. ; Lutz, Jean-Robert ; Ma, K. ; Ma, R. ; Madagodahettige-Don, D.M. ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, D.P. ; Maire, Antonin ; Makhlyueva, I. ; Mal’Kevich, Dmitry ; Malaev, Mikhail ; Malagalage, K.J. ; Maldonado Cervantes, Ivonne Alicia ; Malek, M. ; Malkiewicz, T. ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Mangotra, L. ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Mao, Yaxian ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marín, Ana ; Martashvili, Irakli ; Martinengo, Paolo ; Martínez Hernández, M.I. ; Martínez Davalos, A. ; Martínez Garcia, Ginés ; Maruyama, Y. ; Marzari Chiesa, A. ; Masciocchi, Silvia ; Masera, Massimo ; Masetti, M. ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastromarco, Mario ; Mastroserio, Annalisa ; Matthews, Z.L. ; Matyja, Adam Tomasz ; Mayani, D. ; Mazza, G. ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mendez Lorenzo, P. ; Meoni, M. ; Mercado Pérez, Jorge ; Mereu, P. ; Miake, Yasuo ; Michalon, A. ; Miftakhov, N. ; Milano, Leonardo ; Milošević, Jovan ; Minafra, F. ; Mischke, André ; Miśkowiec, Dariusz Czesław ; Mitu, C. ; Mizoguchi, K. ; Mlynarz, J. ; Mohanty, Bedangadas ; Molnar, Levente ; Mondal, Mriganka Mouli ; Montaño Zetina, Luis Manuel ; Monteno, M. ; Montes Prado, Esther ; Morando, Maurizio ; Moretto, Sandra ; Morsch, Andreas ; Moukhanova, T. ; Muccifora, Valeria ; Mudnic, Eugen ; Muhuri, Sanjib ; Müller, H. ; Munhoz, Marcelo Gameiro ; Munoz, J. ; Musa, Luciano ; Musso, A. ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Navach, F. ; Navin, S. ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nazarov, G. ; Nedosekin, Alexander ; Nendaz, F. ; Newby, J. ; Nianine, A. ; Nicassio, Maria ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikolic, V. ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, B.S. ; Nilsson, M.S. ; Noferini, Francesco ; Nomokonov, Petr V. ; Nooren, Gerardus ; Novitzky, Norbert ; Nyatha, A. ; Nygaard, C. ; Nyiri, A. ; Nystrand, Joakim Ingemar ; Ochirov, A. ; Odyniec, G. ; Oeschler, Helmut ; Oinonen, M. ; Okada, K. ; Okada, Y. ; Oldenburg, Markus D. ; Oleniacz, Janusz ; Oppedisano, Chiara ; Orsini, F. ; Ortiz Velasquez, Antonio ; Ortona, G. ; Oskarsson, Anders Nils Erik ; Osmic, F. ; Österman, L. ; Ostrowski, P. ; Otterlund, I. ; Otwinowski, Jacek Tomasz ; Øvrebekk, G. ; Oyama, Ken ; Ozawa, K. ; Pachmayer, Yvonne C. ; Pachr, Miloš ; Padilla, F. ; Pagano, Paola ; Paić, Guy ; Painke, F. ; Pajares Vales, Carlos ; Pal, S. ; Pal, Susanta Kumar ; Palaha, A. ; Palmeri, A. ; Panse, R. ; Papikyan, Vardanush ; Pappalardo, Giuseppe Salvatore ; Park, WooJin ; Pastirčák, B. ; Pastore, C. ; Paticchio, Vincenzo ; Pavlinov, A. ; Pawlak, Tomasz Jan ; Peitzmann, Thomas ; Pepato, A. ; Pereira, H. ; Peressounko, D. ; Pérez, C. ; Perini, D. ; Perrino, D. ; Peryt, Wiktor Stanislaw ; Peschek, J. ; Pesci, A. ; Peskov, Vladimir ; Pestov, Yury N. ; Peters, A.J. ; Petráček, Vojtech ; Petridis, Athanasios ; Petris, M. ; Petrov, P. ; Petrovici, Mihai A. ; Petta, Catia ; Peyré, J. ; Piano, Stefano ; Piccotti, A. ; Pikna, Miroslav ; Pillot, Philippe ; Pinazza, Ombretta ; Pinsky, Lawrence ; Pitz, N. ; Piuz, F. ; Platt, R. ; Płoskoń, Mateusz ; Pluta, Jan Marian ; Pocheptsov, T. ; Pochybova, Sona ; Podesta Lerma, P.L.M. ; Poggio, F. ; Poghosyan, Martin G. ; Polák, K. ; Polichtchouk, Boris ; Polozov, P. ; Polyakov, V. ; Pommeresch, B. ; Pop, Amalia ; Posa, F. ; Pospíšil, V. ; Potukuchi, B. ; Pouthas, J. ; Prasad, Sidharth Kumar ; Preghenella, Roberto ; Prino, Francesco ; Pruneau, Claude A. ; Pshenichnov, Igor A. ; Puddu, Giovanna ; Pujahari, Prabhat Ranjan ; Pulvirenti, A. ; Punin, A. ; Punin, Valery ; Putiš, M. ; Putschke, Jörn H. ; Quercigh, E. ; Rachevski, Alexandre ; Rademakers, A. ; Radomski, S. ; Räihä, T.S. ; Rak, Jan ; Rakotozafindrabe, Andry Malala ; Ramello, Luciano ; Ramírez Reyes, A. ; Rammler, M. ; Raniwala, Rashmi ; Raniwala, Sudhir ; Räsänen, Sami Sakari ; Rashevskaya, I. ; Rath, S. ; Read, Kenneth Francis ; Real, Jean-Sébastien ; Redlich, Krzysztof ; Renfordt, Rainer Arno Ernst ; Reolon, Anna Rita ; Reshetin, Andrey ; Rettig, Felix Vincenz ; Revol, Jean-Pierre ; Reygers, Klaus ; Ricaud, H. ; Riccati, L. ; Ricci, Renato Angelo ; Richter, Matthias Rudolph ; Riedler, Petra ; Riegler, Werner ; Riggi, Francesco ; Rivetti, Angelo ; Rodrı́guez Cahuantzi, Mario ; Røed, Ketil ; Röhrich, Dieter ; Román López, S. ; Romita, Rosa ; Ronchetti, Federico ; Rosinský, P. ; Rosnet, Philippe ; Rossegger, S. ; Rossi, Andrea ; Roukoutakis, Filimon ; Rousseau, S. ; Roy, Christelle Sophie ; Roy, Pradip Kumar ; Rubio-Montero, A.J. ; Rui, Rinaldo ; Rusanov, I. ; Russo, G. ; Ryabinkin, Evgeny ; Rybicki, Andrzej ; Sadovskiy, Sergey ; Šafařík, Karel ; Sahoo, Raghunath ; Saini, Jogender ; Saiz, P. ; Sakata, D. ; Salgado, Carlos A. ; Salgueiro Domingues da Silva, R. ; Salur, Sevil ; Samanta, T. ; Sambyal, Sanjeev Singh ; Samsonov, Vladimir ; Šándor, Ladislav ; Sandoval, Andres ; Sano, Masato ; Sano, S. ; Santo, R. ; Santoro, R. ; Sarkamo, J. ; Saturnini, P. ; Scapparone, Eugenio ; Scarlassara, Fernando ; Scharenberg, Rolf Paul ; Schiaua, Claudiu Cornel ; Schicker, Rainer ; Schindler, H. ; Schmidt, Christian Joachim ; Schmidt, Hans Rudolf ; Schossmaier, K. ; Schreiner, S. ; Schuchmann, Simone ; Schukraft, Jürgen ; Schutz, Yves Roland ; Schwarz, Kilian ; Schweda, Kai ; Scioli, Gilda ; Scomparin, Enrico ; Scott, P.A. ; Segato, G. ; Semenov, D. ; Senyukov, Serhiy ; Seo, Jeewon ; Serci, S. ; Serkin, L. ; Serradilla, Eulogio ; Sevcenco, Adrian ; Sgura, I. ; Shabratova, G. ; Shahoyan, Ruben ; Sharkov, G. ; Sharma, Natasha ; Sharma, S. ; Shigaki, Kenta ; Shimomura, Maya ; Shtejer, Katherin ; Sibiriak, Yury ; Siciliano, M. ; Sicking, E. ; Siddi, E. ; Siemiarczuk, Teodor ; Silenzi, A. ; Silvermyr, David Olle Rickard ; Simili, E. ; Simonetti, Giuseppe ; Singaraju, Rama Narayana ; Singh, R. ; Singhal, Vikas ; Sinha, Bikash ; Sinha, Tinku ; Sitar, Branislav ; Sitta, Mario ; Skaali, Toralf Bernhard ; Skjerdal, K. ; Smakal, R. ; Smirnov, N. ; Snellings, Raimond ; Snow, H. ; Søgaard, C. ; Soloviev, A. ; Soltveit, H.K. ; Soltz, Ron ; Sommer, W. ; Son, C.W. ; Son, H. ; Song, M. ; Soos, C. ; Soramel, Francesca ; Soyk, D. ; Spyropoulou-Stassinaki, Martha ; Srivastava, Brijesh Kumar ; Stachel, Johanna ; Staley, F. ; Stan, E. ; Stefanek, Grzegorz ; Stefanini, G. ; Steinbeck, T. ; Stenlund, Evert Anders ; Steyn, Gideon Francois ; Stocco, Diego ; Stock, Reinhard ; Stolpovsky, P. ; Strmen, Peter ; Suaide, Alexandre Alarcon do Passo ; Subieta Vasquez, Martin Alfonso ; Sugitate, Toru ; Suire, Christophe Pierre ; Šumbera, Michal ; Šuša, Tatjana ; Swoboda, D. ; Symons, J. ; Toledo, Alejandro Szanto de ; Szarka, Imrich ; Szostak, A. ; Szuba, M. ; Tadel, M. ; Tagridis, C. ; Takahara, A. ; Takahashi, Jun ; Tanabe, R. ; Tapia Takaki, Jesus Daniel ; Taureg, H. ; Tauro, Arturo ; Tavlet, M. ; Tejeda Muñoz, Guillermo ; Telesca, Adriana ; Terrevoli, Cristina ; Thäder, Jochen ; Tieulent, Raphael Noel ; Tlusty, David ; Toia, Alberica ; Tolyhy, T. ; Torcato de Matos, C. ; Torii, H. ; Torralba, G. ; Toscano, L. ; Tosello, F. ; Tournaire, A. ; Traczyk, T. ; Tribedy, Prithwish ; Tröger, G. ; Truesdale, David Christopher ; Trzaska, Wladyslaw Henryk ; Tsiledakis, G. ; Tsilis, E. ; Tsuji, Tomoya ; Tumkin, Alexandr ; Turrisi, Rosario ; Turvey, A. ; Tveter, Trine Spedstad ; Tydesjö, H. ; Tywoniuk, K. ; Ulery, Jason Glyndwr ; Ullaland, Kjetil ; Uras, Antonio ; Urbán, J. ; Urciuoli, G.M. ; Usai, Gianluca ; Vacchi, A. ; Vala, Martin ; Valencia Palomo, Lizardo ; Vallero, Sara ; Kolk, Naomi van der ; Vyvre, Pierre vande ; Leeuwen, Marco van ; Vannucci, L. ; Vargas Treviño, Maria Aurora Diozcora ; Varma, Raghava ; Vasiliev, Andrey ; Vassiliev, Iouri ; Vasileiou, Maria ; Vechernin, Vladimir ; Venaruzzo, Massimo ; Vercellin, Ermanno ; Vergara, S. ; Vernet, Renaud ; Verweij, Marta ; Vetlitskiy, I. ; Vicković, Linda ; Viesti, Giuseppe ; Vikhlyantsev, O. ; Vilakazi, Zabulon ; Villalobos Baillie, Orlando ; Vinogradov, Alexander A. ; Vinogradov, Leonid ; Vinogradov, Yury I. ; Virgili, Tiziano ; Viyogi, Yogendra P. ; Vodopianov, A. ; Voloshin, Kirill ; Voloshin, Sergei ; Volpe, Giacomo ; Haller, Barthélémy von ; Vranić, Danilo ; Vrláková, Janka ; Vulpescu, Bogdan ; Wagner, Boris ; Wagner, V. ; Wallet, L. ; Wan, R. ; Wang, D. ; Wang, Y. ; Wang, Y. ; Watanabe, K. ; Wen, Q. ; Wessels, J. ; Westerhoff, Uwe ; Wiechula, Jens ; Wikne, Jon ; Wilk, A. ; Wilk, Grzegorz Andrzej ; Williams, M. Crispin S. ; Willis, N. ; Windelband, Bernd ; Xu, C. ; Yang, C. ; Yang, H. ; Yasnopolskiy, S. ; Yermia, F. ; Yi, J. ; Yin, Zhongbao ; Yokoyama, Hiroki ; Yoo, In-Kwon ; Yuan, X. ; Yurevich, V. ; Yushmanov, Igor E. ; Zabrodin, E. ; Zagreev, B. ; Zalite, A. ; Zampolli, Chiara ; Zanevsky, Yuri V. ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zbroszczyk, Hanna Paulina ; Zelnicek, P. ; Zenin, A. ; Zepeda, A. ; Zgura, I. ; Zhalov, Mikhail ; Zhang, X. ; Zhou, D. ; Zhou, S. ; Zhu, J. ; Zichichi, Antonino ; Zinchenko, A. ; Zinovjev, Gennady M. ; Zoccarato, Y. ; Zycháček, V. ; Zynovyev, M.
The inclusive charged particle transverse momentum distribution is measured in proton–proton collisions at s=900 GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region (|η|<0.8) over the transverse momentum range 0.15<pT<10 GeV/c. The correlation between transverse momentum and particle multiplicity is also studied. Results are presented for inelastic (INEL) and non-single-diffractive (NSD) events. The average transverse momentum for |η|<0.8 is 〈pT〉INEL=0.483±0.001 (stat.)±0.007 (syst.) GeV/c and 〈pT〉NSD=0.489±0.001 (stat.)±0.007 (syst.) GeV/c, respectively. The data exhibit a slightly larger 〈pT〉 than measurements in wider pseudorapidity intervals. The results are compared to simulations with the Monte Carlo event generators PYTHIA and PHOJET.
FIAS Scientific Report 2013
(2014)
FIAS Scientific Report 2012
(2013)
FIAS Scientific Report 2011
(2012)
FIAS Scientific Report 2014
(2015)
FIAS Scientific Report 2009
(2010)
In this Annual Report we present some of the ongoing activities of FIAS and of the associated graduate
school, the “Frankfurt International Graduate School for Science” (FIGSS) in the year 2009. The main part of the Report consists of a collection of short reports describing the research projects of scientists working at or associated with FIAS.
Measurement of ϒ(1S) elliptic flow at forward rapidity in Pb-Pb collisions at √sNN = 5.02 TeV
(2019)
The first measurement of the ϒ(1S) elliptic flow coefficient (v2) is performed at forward rapidity (2.5 < y < 4) in Pb–Pb collisions at √sNN = 5.02 TeV with the ALICE detector at the LHC. The results are obtained with the scalar product method and are reported as a function of transverse momentum (pT) up to 15 GeV/c in the 5%–60% centrality interval. The measured Υ(1S)v2 is consistent with 0 and with the small positive values predicted by transport models within uncertainties. The v2 coefficient in 2 < pT < 15 GeV/c is lower than that of inclusive J/ψ mesons in the same pT interval by 2.6 standard deviations. These results, combined with earlier suppression measurements, are in agreement with a scenario in which the Υ(1S) production in Pb–Pb collisions at LHC energies is dominated by dissociation limited to the early stage of the collision, whereas in the J/ψ case there is substantial experimental evidence of an additional regeneration component.
An invariant differential cross section measurement of inclusive π0 and η meson production at mid-rapidity in pp collisions at s√=8 TeV was carried out by the ALICE experiment at the LHC. The spectra of π0 and η mesons were measured in transverse momentum ranges of 0.3<p T <35 GeV/c and 0.5<p T <35 GeV/c , respectively. Next-to-leading order perturbative QCD calculations using fragmentation functions DSS14 for the π0 and AESSS for the η overestimate the cross sections of both neutral mesons, although such calculations agree with the measured η/π0 ratio within uncertainties. The results were also compared with PYTHIA 8.2 predictions for which the Monash 2013 tune yields the best agreement with the measured neutral meson spectra. The measurements confirm a universal behavior of the η/π0 ratio seen for NA27, PHENIX and ALICE data for pp collisions from s√=27.5 GeV to s√=8 TeV within experimental uncertainties. A relation between the π0 and η production cross sections for pp collisions at s√=8 TeV is given by m T scaling for p T >3.5 GeV/c . However, a deviation from this empirical scaling rule is observed for transverse momenta below p T <3.5 GeV/c in the η/π0 ratio with a significance of 6.2σ.
We report about the properties of the underlying event measured with ALICE at the LHC in pp and p−Pb collisions at sNN−−−√=5.02 TeV. The event activity, quantified by charged-particle number and summed-pT densities, is measured as a function of the leading-particle transverse momentum (ptrigT). These quantities are studied in three azimuthal-angle regions relative to the leading particle in the event: toward, away, and transverse. Results are presented for three different pT thresholds (0.15, 0.5, and 1 GeV/c) at mid-pseudorapidity (|η|<0.8). The event activity in the transverse region, which is the most sensitive to the underlying event, exhibits similar behaviour in both pp and p−Pb collisions, namely, a steep increase with ptrigT for low ptrigT, followed by a saturation at ptrigT≈5 GeV/c. The results from pp collisions are compared with existing measurements at other centre-of-mass energies. The quantities in the toward and away regions are also analyzed after the subtraction of the contribution measured in the transverse region. The remaining jet-like particle densities are consistent in pp and p−Pb collisions for ptrigT>10 GeV/c, whereas for lower ptrigT values the event activity is slightly higher in p−Pb than in pp collisions. The measurements are compared with predictions from the PYTHIA 8 and EPOS LHC Monte Carlo event generators.
The ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y|<0.8 and transverse momentum 1<pT<10 GeV/c, in pp collisions at s√= 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD calculations agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, σb→e=3.47±0.40(stat)+1.12−1.33(sys)±0.07(norm)μb, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total bb¯ production cross section, σbb¯=130±15.1(stat)+42.1−49.8(sys)+3.4−3.1(extr)±2.5(norm)±4.4(BR)μb.
FIAS Scientific Report 2010
(2011)
In the year 2010 the Frankfurt Institute for Advanced Studies has successfully continued to follow its agenda to pursue theoretical research in the natural sciences. As stipulated in its charter, FIAS closely collaborates with extramural research institutions, like the Max Planck Institute for Brain Research in Frankfurt and the GSI Helmholtz Center for Heavy Ion Research, Darmstadt and with research groups at the science departments of Goethe University. The institute also engages in the training of young researchers and the education of doctoral students. This Annual Report documents how these goals have been pursued in the year 2010. Notable events in the scientific life of the Institute will be presented, e.g., teaching activities in the framework of the Frankfurt International Graduate School for Science (FIGSS), colloquium schedules, conferences organized by FIAS, and a full bibliography of publications by authors affiliated with FIAS. The main part of the Report consists of short one-page summaries describing the scientific progress reached in individual research projects in the year 2010...
The azimuthal (Δφ) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p−Pb collisions at sNN−−−√=5.02 TeV. Results are reported for electrons with transverse momentum 4<pT<16 GeV/c and pseudorapidity |η|<0.6. The associated charged particles are selected with transverse momentum 1<pT<7 GeV/c, and relative pseudorapidity separation with the leading electron |Δη|<1. The correlation measurements are performed to study and characterize the fragmentation and hadronization of heavy quarks. The correlation structures are fitted with a constant and two von Mises functions to obtain the baseline and the near- and away-side peaks, respectively. The results from p−Pb collisions are compared with those from pp collisions to study the effects of cold nuclear matter. In the measured trigger electron and associated particle kinematic regions, the two collision systems give consistent results. The Δφ distribution and the peak observables in pp and p−Pb collisions are compared with calculations from various Monte Carlo event generators.
The first measurement of the e+e− pair production at low lepton pair transverse momentum (pT,ee) and low invariant mass (mee) in non-central Pb−Pb collisions at sNN−−−√=5.02 TeV at the LHC is presented. The dielectron production is studied with the ALICE detector at midrapidity (|ηe|<0.8) as a function of invariant mass (0.4≤mee<2.7 GeV/c2) in the 50−70% and 70−90% centrality classes for pT,ee<0.1 GeV/c, and as a function of pT,ee in three mee intervals in the most peripheral Pb−Pb collisions. Below a pT,ee of 0.1 GeV/c, a clear excess of e+e− pairs is found compared to the expectations from known hadronic sources and predictions of thermal radiation from the medium. The mee excess spectra are reproduced, within uncertainties, by different predictions of the photon−photon production of dielectrons, where the photons originate from the extremely strong electromagnetic fields generated by the highly Lorentz-contracted Pb nuclei. Lowest-order quantum electrodynamic (QED) calculations, as well as a model that takes into account the impact-parameter dependence of the average transverse momentum of the photons, also provide a good description of the pT,ee spectra. The measured ⟨p2T,ee⟩−−−−−√ of the excess pT,ee spectrum in peripheral Pb−Pb collisions is found to be comparable to the values observed previously at RHIC in a similar phase-space region.
The measurement of the production of charm jets, identified by the presence of a D0 meson in the jet constituents, is presented in proton-proton collisions at centre-of-mass energies of s√ = 5.02 and 13 TeV with the ALICE detector at the CERN LHC. The D0 mesons were reconstructed from their hadronic decay D0→K−π+ and the respective charge conjugate. Jets were reconstructed from D0-meson candidates and charged particles using the anti-kT algorithm, in the jet transverse momentum range 5<pT;chjet<50 GeV/c, pseudorapidity |ηjet|<0.9−R, and with the jet resolution parameters R = 0.2, 0.4, 0.6. The distribution of the jet momentum fraction carried by a D0 meson along the jet axis (zch||) was measured in the range 0.4<zch||<1.0 in four ranges of the jet transverse momentum. Comparisons of results for different collision energies and jet resolution parameters are also presented. The measurements are compared to predictions from Monte Carlo event generators based on leading-order and next-to-leading-order perturbative quantum chromodynamics calculations. A generally good description of the main features of the data is obtained in spite of a few discrepancies at low pT;chjet. Measurements were also done for R=0.3 at s√ = 5.02 TeV and are shown along with their comparisons to theoretical predictions in an appendix to this paper.
The azimuthal (Δφ) correlation distributions between heavy-flavor decay electrons and associated charged particles are measured in pp and p−Pb collisions at sNN−−−√=5.02 TeV. Results are reported for electrons with transverse momentum 4<pT<16 GeV/c and pseudorapidity |η|<0.6. The associated charged particles are selected with transverse momentum 1<pT<7 GeV/c, and relative pseudorapidity separation with the leading electron |Δη|<1. The correlation measurements are performed to study and characterize the fragmentation and hadronization of heavy quarks. The correlation structures are fitted with a constant and two von Mises functions to obtain the baseline and the near- and away-side peaks, respectively. The results from p−Pb collisions are compared with those from pp collisions to study the effects of cold nuclear matter. In the measured trigger electron and associated particle kinematic regions, the two collision systems give consistent results. The Δφ distribution and the peak observables in pp and p−Pb collisions are compared with calculations from various Monte Carlo event generators.
A newly developed observable for correlations between symmetry planes, which characterize the direction of the anisotropic emission of produced particles, is measured in Pb-Pb collisions at sNN−−−√=2.76 TeV with ALICE. This so-called Gaussian Estimator allows for the first time the study of these quantities without the influence of correlations between different flow amplitudes. The centrality dependence of various correlations between two, three and four symmetry planes is presented. The ordering of magnitude between these symmetry plane correlations is discussed and the results of the Gaussian Estimator are compared with measurements of previously used estimators. The results utilizing the new estimator lead to significantly smaller correlations than reported by studies using the Scalar Product method. Furthermore, the obtained symmetry plane correlations are compared to state-of-the-art hydrodynamic model calculations for the evolution of heavy-ion collisions. While the model predictions provide a qualitative description of the data, quantitative agreement is not always observed, particularly for correlators with significant non-linear response of the medium to initial state anisotropies of the collision system. As these results provide unique and independent information, their usage in future Bayesian analysis can further constrain our knowledge on the properties of the QCD matter produced in ultrarelativistic heavy-ion collisions.
Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons v2{ΨSP} in collisions of Pb ions at center-of-mass energy per nucleon-nucleon pair sNN−−−√=2.76 TeV and Xe ions at sNN−−−√=5.44 TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum. The ratio between v2{ΨSP} and the elliptic flow coefficient relative to the participant plane v2{4}, estimated using four-particle correlations, deviates by up to 20% from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models of initial state fluctuations. A significant transverse momentum dependence of the ratio v2{ΨSP}/v2{4} is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state fluctuations. The ratios of v2{ΨSP} and v2{4} to the corresponding initial state eccentricities for Xe-Xe and Pb-Pb collisions at similar initial entropy density show a difference of (7.0±0.9)% with an additional variation of +1.8% when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark-gluon plasma.
This article presents new measurements of the fragmentation properties of jets in both proton-proton (pp) and heavy-ion collisions with the ALICE experiment at the Large Hadron Collider (LHC). We report distributions of the fraction zr of transverse momentum carried by subjets of radius r within jets of radius R. Charged-particle jets are reconstructed at midrapidity using the anti-kT algorithm with jet radius R=0.4, and subjets are reconstructed by reclustering the jet constituents using the anti-kT algorithm with radii r=0.1 and r=0.2. In proton-proton collisions, we measure both the inclusive and leading subjet distributions. We compare these measurements to perturbative calculations at next-to-leading logarithmic accuracy, which suggest a large impact of threshold resummation and hadronization effects on the zr distribution. In heavy-ion collisions, we measure the leading subjet distributions, which allow access to a region of harder jet fragmentation than has been probed by previous measurements of jet quenching via hadron fragmentation distributions. The zr distributions enable extraction of the parton-to-subjet fragmentation function and allow for tests of the universality of jet fragmentation functions in the quark-gluon plasma (QGP). We find indications that there is a turnover in the ratio between the distributions in Pb-Pb and pp collisions as zr→1, exposing qualitatively new possibilities to disentangle competing jet quenching mechanisms. By comparing our results to theoretical calculations based on an independent extraction of the parton-to-jet fragmentation function, we find consistency with the universality of jet fragmentation and no indication of factorization breaking in the QGP.
The production yields of non-prompt Ds+ mesons, namely Ds+ mesons from beauty-hadron decays, were measured for the first time as a function of the transverse momentum (pT) at midrapidity (|y|<0.5) in central and semi-central Pb−Pb collisions at a centre-of-mass energy per nucleon pair sNN−−−√=5.02 TeV with the ALICE experiment at the LHC. The Ds+ mesons and their charge conjugates were reconstructed from the hadronic decay channel Ds+→ϕπ+, with ϕ→K−K+, in the 4<pT<36 GeV/c and 2<pT<24 GeV/c intervals for the 0−10% and 30−50% centrality classes, respectively. The measured yields of non-prompt Ds+ mesons are compared to those of prompt Ds+ and non-prompt D0 mesons by calculating the ratios of the production yields in Pb−Pb collisions and the nuclear modification factor RAA. The ratio between the RAA of non-prompt Ds+ and prompt Ds+ mesons, and that between the RAA of non-prompt Ds+ and non-prompt D0 mesons in central Pb−Pb collisions are found to be on average higher than unity in the 4<pT<12 GeV/c interval with a statistical significance of about 1.6σ and 1.7σ, respectively. The measured RAA ratios are compared with the predictions of theoretical models of heavy-quark transport in a hydrodynamically expanding QGP that incorporate hadronisation via quark recombination.
Charmonium production in pp collisions at center-of-mass energy of s√ = 13 TeV and p-Pb collisions at center-of-mass energy per nucleon pair of sNN−−−√ = 8.16 TeV is studied as a function of charged-particle pseudorapidity density with ALICE. Ground and excited charmonium states (J/ψ, ψ(2S)) are measured from their dimuon decays in the interval of rapidity in the center-of-mass frame 2.5<ycms<4.0 for pp collisions, and 2.03<ycms<3.53 and −4.46<ycms<−2.96 for p-Pb collisions. The charged-particle pseudorapidity density is measured around midrapidity (|η|<1.0). In pp collisions, the measured charged-particle multiplicity extends to about six times the average value, while in p-Pb collisions at forward (backward) rapidity a multiplicity corresponding to about three (four) times the average is reached. The ψ(2S) yield increases with the charged-particle pseudorapidity density. The ratio of ψ(2S) over J/ψ yield does not show a significant multiplicity dependence in either colliding system, suggesting a similar behavior of J/ψ and ψ(2S) yields with respect to charged-particle pseudorapidity density. The results are also compared with model calculations.
The first experimental information on the strong interaction between Λ and Ξ− strange baryons is presented in this Letter. The correlation function of Λ−Ξ− and Λ¯¯¯¯−Ξ¯¯¯¯+ pairs produced in high-multiplicity proton-proton (pp) collisions at s√ = 13 TeV at the LHC is measured as a function of the relative momentum of the pair. The femtoscopy method is used to calculate the correlation function, which is then compared with theoretical expectations obtained using a meson exchange model, chiral effective field theory, and Lattice QCD calculations close to the physical point. Data support predictions of small scattering parameters while discarding versions with large ones, thus suggesting a weak Λ−Ξ− interaction. The limited statistical significance of the data does not yet allow one to constrain the effects of coupled channels like Σ−Ξ and N−Ω.
Two-particle transverse momentum differential correlators, recently measured in Pb--Pb collisions at energies available at the CERN Large Hadron Collider (LHC), provide an additional tool to gain insights into particle production mechanisms and infer transport properties, such as the ratio of shear viscosity to entropy density, of the medium created in Pb-Pb collisions. The longitudinal long-range correlations and the large azimuthal anisotropy measured at low transverse momenta in small collision systems, namely pp and p-Pb, at LHC energies resemble manifestations of collective behaviour. This suggests that locally equilibrated matter may be produced in these small collision systems, similar to what is observed in Pb-Pb collisions. In this work, the same two-particle transverse momentum differential correlators are exploited in pp and p-Pb collisions at √s=7 TeV and sNN−−−√=5.02 TeV, respectively, to seek evidence for viscous effects. Specifically, the strength and shape of the correlators are studied as a function of the produced particle multiplicity to identify evidence for longitudinal broadening that might reveal the presence of viscous effects in these smaller systems. The measured correlators and their evolution from pp and p--Pb to Pb--Pb collisions are additionally compared to predictions from Monte Carlo event generators, and the potential presence of viscous effects is discussed.
Jet-like correlations with respect to K0S and Λ (Λ‾) in pp and Pb–Pb collisions at √sNN = 5.02 TeV
(2022)
Two-particle correlations with K0S, Λ/Λ¯, and charged hadrons as trigger particles in the transverse momentum range 8<pT,trig<16 GeV/c, and associated charged particles within 1<pT,assoc<8 GeV/c, are studied at mid-rapidity in pp and central Pb-Pb collisions at a centre-of-mass energy per nucleon-nucleon collision sNN−−−√=5.02 TeV with the ALICE detector at the LHC. After subtracting the contributions of the flow background, the per-trigger yields are extracted on both the near and away sides, and the ratio in Pb-Pb collisions with respect to pp collisions (IAA) is computed. The per-trigger yield in Pb-Pb collisions on the away side is strongly suppressed to the level of IAA≈0.6 for pT,assoc>3 GeV/c as expected from strong in-medium energy loss, while an enhancement develops at low pT,assoc on both the near and away sides, reaching IAA≈1.8 and 2.7 respectively. These findings are in good agreement with previous ALICE measurements from two-particle correlations triggered by neutral pions (π0-h) and charged hadrons (h-h) in Pb-Pb collisions at sNN−−−√=2.76 TeV. Moreover, the correlations with K0S mesons and Λ/Λ¯ baryons as trigger particles are compared to those of inclusive charged hadrons. The results are compared with the predictions of Monte Carlo models.
The measurement of the production of deuterons, tritons and 3He and their antiparticles in Pb-Pb collisions at sNN−−−√=5.02 TeV is presented in this article. The measurements are carried out at midrapidity (|y|< 0.5) as a function of collision centrality using the ALICE detector. The pT-integrated yields, the coalescence parameters and the ratios to protons and antiprotons are reported and compared with nucleosynthesis models. The comparison of these results in different collision systems at different centre-of-mass collision energies reveals a suppression of nucleus production in small systems. In the Statistical Hadronisation Model framework, this can be explained by a small correlation volume where the baryon number is conserved, as already shown in previous fluctuation analyses. However, a different size of the correlation volume is required to describe the proton yields in the same data sets. The coalescence model can describe this suppression by the fact that the wave functions of the nuclei are large and the fireball size starts to become comparable and even much smaller than the actual nucleus at low multiplicities.
The pseudorapidity density of charged particles with minimum transverse momentum (pT) thresholds of 0.15, 0.5, 1, and 2 GeV/c was measured in pp collisions at centre-of-mass energies of √s = 5.02 and 13 TeV with the ALICE detector. The study is carried out for inelastic collisions with at least one primary charged particle having a pseudorapidity (η) within ±0.8 and pT larger than the corresponding threshold. The measurements were also performed for inelastic and non-single-diffractive events as well as for inelastic events with at least one charged particle having |η| < 1 in pp collisions at √s = 5.02 TeV for the first time at the LHC. The measurements are compared to the PYTHIA 6, PYTHIA 8, and EPOS-LHC models. In general, the models describe the pseudorapidity dependence of particle production well, however, discrepancies are observed for event classes including diffractive events and for the highest transverse momentum threshold (pT > 2 GeV/c), highlighting the importance of such measurements for tuning event generators. The new measurements agree within uncertainties with results from the ATLAS and CMS experiments.
First measurement of 𝚲+c production down to 𝑝T = 0 in pp and p–Pb collisions at √𝑠NN = 5.02 TeV
(2023)
The production of prompt Λ+c baryons has been measured at midrapidity in the transverse momentum interval 0<pT<1 GeV/c for the first time, in pp and p-Pb collisions at a centre-of-mass energy per nucleon-nucleon collision sNN−−−√=5.02 TeV. The measurement was performed in the decay channel Λ+c→pK0S by applying new decay reconstruction techniques using a Kalman-Filter vertexing algorithm and adopting a machine-learning approach for the candidate selection. The pT-integrated Λ+c production cross sections in both collision systems were determined and used along with the measured yields in Pb-Pb collisions to compute the pT-integrated nuclear modification factors RpPb and RAA of Λ+c baryons, which are compared to model calculations that consider nuclear modification of the parton distribution functions. The Λ+c/D0 baryon-to-meson yield ratio is reported for pp and p-Pb collisions. Comparisons with models that include modified hadronisation processes are presented, and the implications of the results on the understanding of charm hadronisation in hadronic collisions are discussed. A significant (3.7σ) modification of the mean transverse momentum of Λ+c baryons is seen in p-Pb collisions with respect to pp collisions, while the pT-integrated Λ+c/D0 yield ratio was found to be consistent between the two collision systems within the uncertainties.
The first measurement of event-by-event antideuteron number fluctuations in high energy heavy-ion collisions is presented. The measurements are carried out at midrapidity (|η|<0.8) as a function of collision centrality in Pb−Pb collisions at sNN−−−√=5.02 TeV using the ALICE detector. A significant negative correlation between the produced antiprotons and antideuterons is observed in all collision centralities. The results are compared with coalescence calculations, which fail to describe the measurement, in particular if a correlated production of protons and neutrons is assumed. Thermal-statistical model calculations describe the data within uncertainties only for correlation volumes that are different with respect to those describing proton yields and a similar measurement of net-proton number fluctuations.
The transverse-momentum (pT) spectra of K∗(892)0 and ϕ(1020) measured with the ALICE detector up to pT = 16 GeV/c in the rapidity range −1.2<y<0.3, in p-Pb collisions at center-of-mass energy per nucleon-nucleon collision sNN−−−√ = 5.02 TeV are presented as a function of charged particle multiplicity and rapidity. The measured pT distributions show a dependence on both multiplicity and rapidity at low pT whereas no significant dependence is observed at high pT. A rapidity dependence is observed in the pT-integrated yield (dN/dy), whereas the mean transverse momentum (⟨pT⟩) shows a flat behavior as a function of rapidity. The rapidity asymmetry (Yasym) at low pT ( < 5 GeV/c) is more significant for higher multiplicity classes. At high pT, no significant rapidity asymmetry is observed in none of the multiplicity classes. Both K∗(892)0 and ϕ(1020) show similar Yasym. The nuclear modification factor (QCP) as a function of pT shows a Cronin-like enhancement at intermediate pT, which is more prominent at higher rapidities (Pb-going direction) and in higher multiplicity classes. At high pT (> 5 GeV/c), the QCP values are greater than unity and no significant rapidity dependence is observed.
Measurement of the J/ψ polarization with respect to the event plane in Pb–Pb collisions at the LHC
(2022)
The polarization of inclusive J/ψ produced in Pb-Pb collisions at sNN−−−√=5.02 TeV at the LHC was studied by ALICE in the dimuon channel, via the measurement of the angular distribution of its decay products. The study was performed in the rapidity region 2.5<y<4, for three transverse momentum intervals (2<pT<4, 4<pT<6, 6<pT<10 GeV/c) and as a function of the centrality of the collision for 2<pT<6 GeV/c. For the first time, the polarization was measured with respect to the event plane of the collision, by considering the angle between the positive-charge decay muon in the J/ψ rest frame and the axis perpendicular to the event-plane vector in the laboratory system. A small transverse polarization is measured, with a significance reaching 3.9σ at low pT and for intermediate centrality values. The polarization could be connected with the existence of a strong magnetic field in the early stage of quark-gluon plasma formation in Pb-Pb collisions, as well as with its behaviour as a rotating fluid with large vorticity.
Investigation of K+K− interactions via femtoscopy in Pb−Pb collisions at √sNN = 2.76 TeV at the LHC
(2022)
Femtoscopic correlations of non-identical charged kaons (K+K−) are studied in Pb−Pb collisions at a center-of-mass energy per nucleon−nucleon collision sNN−−−√=2.76 TeV by ALICE at the LHC. One-dimensional K+K− correlation functions are analyzed in three centrality classes and eight intervals of particle-pair transverse momentum. The Lednický and Luboshitz interaction model used in the K+K− analysis includes the final-state Coulomb interactions between kaons and the final-state interaction through a0(980) and f0(980) resonances. The mass of f0(980) and coupling were extracted from the fit to K+K− correlation functions using the femtoscopic technique for the first time. The measured mass and width of the f0(980) resonance are consistent with other published measurements. The height of the ϕ(1020) meson peak present in the K+K− correlation function rapidly decreases with increasing source radius, qualitatively in agreement with an inverse volume dependence. A phenomenological fit to this trend suggests that the ϕ(1020) meson yield is dominated by particles produced directly from the hadronization of the system. The small fraction subsequently produced by FSI could not be precisely quantified with data presented in this paper and will be assessed in future work.
This article reports measurements of the angle between differently defined jet axes in pp collisions at s√=5.02 TeV carried out by the ALICE Collaboration. Charged particles at midrapidity are clustered into jets with resolution parameters R=0.2 and 0.4. The jet axis, before and after Soft Drop grooming, is compared to the jet axis from the Winner-Takes-All (WTA) recombination scheme. The angle between these axes, ΔRaxis, probes a wide phase space of the jet formation and evolution, ranging from the initial high-momentum-transfer scattering to the hadronization process. The ΔRaxis observable is presented for 20<pchjetT<100 GeV/c, and compared to predictions from the PYTHIA 8 and Herwig 7 event generators. The distributions can also be calculated analytically with a leading hadronization correction related to the non-perturbative component of the Collins−Soper−Sterman (CSS) evolution kernel. Comparisons to analytical predictions at next-to-leading-logarithmic accuracy with leading hadronization correction implemented from experimental extractions of the CSS kernel in Drell−Yan measurements are presented. The analytical predictions describe the measured data within 20% in the perturbative regime, with surprising agreement in the non-perturbative regime as well. These results are compatible with the universality of the CSS kernel in the context of jet substructure.
This letter reports measurements which characterize the underlying event associated with hard scatterings at mid-pseudorapidity (|η|<0.8) in pp, p−Pb and Pb−Pb collisions at centre-of-mass energy per nucleon pair, sNN−−−√=5.02 TeV. The measurements are performed with ALICE at the LHC. Different multiplicity classes are defined based on the event activity measured at forward rapidities. The hard scatterings are identified by the leading particle defined as the charged particle with the largest transverse momentum (pT) in the collision and having 8<pT<15 GeV/c. The pT spectra of associated particles (0.5≤pT<6 GeV/c) are measured in different azimuthal regions defined with respect to the leading particle direction: toward, transverse, and away. The associated charged particle yields in the transverse region are subtracted from those of the away and toward regions. The remaining jet-like yields are reported as a function of the multiplicity measured in the transverse region. The measurements show a suppression of the jet-like yield in the away region and an enhancement of high-pT associated particles in the toward region in central Pb−Pb collisions, as compared to minimum-bias pp collisions. These observations are consistent with previous measurements that used two-particle correlations, and with an interpretation in terms of parton energy loss in a high-density quark gluon plasma. These yield modifications vanish in peripheral Pb−Pb collisions and are not observed in either high-multiplicity pp or p−Pb collisions.
This article presents measurements of the groomed jet radius and momentum splitting fraction in pp collisions at s√=5.02 TeV with the ALICE detector at the Large Hadron Collider. Inclusive charged-particle jets are reconstructed at midrapidity using the anti-kT algorithm for transverse momentum 60<pchjetT<80 GeV/c. We report results using two different grooming algorithms: soft drop and, for the first time, dynamical grooming. For each grooming algorithm, a variety of grooming settings are used in order to explore the impact of collinear radiation on these jet substructure observables. These results are compared to perturbative calculations that include resummation of large logarithms at all orders in the strong coupling constant. We find good agreement of the theoretical predictions with the data for all grooming settings considered.
We present the first systematic comparison of the charged-particle pseudorapidity densities for three widely different collision systems, pp, p-Pb, and Pb-Pb, at the top energy of the Large Hadron Collider (sNN−−−√=5.02 TeV) measured over a wide pseudorapidity range (−3.5<η<5), the widest possible among the four experiments at that facility. The systematic uncertainties are minimised since the measurements are recorded by the same experimental apparatus (ALICE). The distributions for p-Pb and Pb-Pb collisions are determined as a function of the centrality of the collisions, while results from pp collisions are reported for inelastic events with at least one charged particle at midrapidity. The charged-particle pseudorapidity densities are, under simple and robust assumptions, transformed to charged-particle rapidity densities. This allows for the calculation and the presentation of the evolution of the width of the rapidity distributions and of a lower bound on the Bjorken energy density, as a function of the number of participants in all three collision systems. We find a decreasing width of the particle production, and roughly a smooth ten fold increase in the energy density, as the system size grows, which is consistent with a gradually higher dense phase of matter.
The inclusive production of the charm-strange baryon Ω0c is measured for the first time via its hadronic decay into Ω−π+ at midrapidity (|y|<0.5) in proton-proton (pp) collisions at the centre-of-mass energy s√=13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2<pT<12 GeV/c. The pT dependence of the Ω0c-baryon production relative to the prompt D0-meson and to the prompt Ξ0c-baryon production is compared to various models that take different hadronisation mechanisms into consideration. In the measured pT interval, the ratio of the pT-integrated cross sections of Ω0c and prompt Λ+c baryons multiplied by the Ω−π+ branching ratio is found to be larger by a factor of about 20 with a significance of about 4σ when compared to e+e− collisions.
Hadronic resonances are used to probe the hadron gas produced in the late stage of heavy-ion collisions since they decay on the same timescale, of the order of 1 to 10 fm/c, as the decoupling time of the system. In the hadron gas, (pseudo)elastic scatterings among the products of resonances that decayed before the kinetic freeze-out and regeneration processes counteract each other, the net effect depending on the resonance lifetime, the duration of the hadronic phase, and the hadronic cross sections at play. In this context, the Σ(1385)± particle is of particular interest as models predict that regeneration dominates over rescattering despite its relatively short lifetime of about 5.5 fm/c. The first measurement of the Σ(1385)± resonance production at midrapidity in Pb-Pb collisions at sNN−−−√=5.02 TeV with the ALICE detector is presented in this Letter. The resonances are reconstructed via their hadronic decay channel, Λπ, as a function of the transverse momentum (pT) and the collision centrality. The results are discussed in comparison with the measured yield of pions and with expectations from the statistical hadronization model as well as commonly employed event generators, including PYTHIA8/Angantyr and EPOS3 coupled to the UrQMD hadronic cascade afterburner. None of the models can describe the data. For Σ(1385)±, a similar behaviour as K∗(892)0 is observed in data unlike the predictions of EPOS3 with afterburner.
This Letter reports on the first measurements of transverse momentum dependent flow angle Ψn and flow magnitude vn fluctuations, determined using new four-particle correlators. The measurements are performed for various centralities in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of sNN−−−√ = 5.02 TeV with ALICE at the CERN Large Hadron Collider. Both flow angle and flow magnitude fluctuations are observed in the presented centrality ranges and are strongest in the most central collisions and for a transverse momentum pT>2 GeV/c. Comparison with theoretical models, including iEBE-VISHNU, MUSIC, and AMPT, show that the measurements exhibit unique sensitivities to the initial state of heavy-ion collisions.
Three-body nuclear forces play an important role in the structure of nuclei and hypernuclei and are also incorporated in models to describe the dynamics of dense baryonic matter, such as in neutron stars. So far, only indirect measurements anchored to the binding energies of nuclei can be used to constrain the three-nucleon force, and if hyperons are considered, the scarce data on hypernuclei impose only weak constraints on the three-body forces. In this work, we present the first direct measurement of the p−p−p and p−p−Λ systems in terms of three-particle mixed moments carried out for pp collisions at s√ = 13 TeV. Three-particle cumulants are extracted from the normalised mixed moments by applying the Kubo formalism, where the three-particle interaction contribution to these moments can be isolated after subtracting the known two-body interaction terms. A negative cumulant is found for the p−p−p system, hinting to the presence of a residual three-body effect while for p−p−Λ the cumulant is consistent with zero. This measurement demonstrates the accessibility of three-baryon correlations at the LHC.
Fluctuation measurements are important sources of information on the mechanism of particle production at LHC energies. This article reports the first experimental results on third-order cumulants of the net-proton distributions in Pb−Pb collisions at a center-of-mass energy sNN−−−√=5.02 TeV recorded by the ALICE detector. The results on the second-order cumulants of net-proton distributions at sNN−−−√=2.76 and 5.02 TeV are also discussed in view of effects due to the global and local baryon number conservation. The results demonstrate the presence of long-range rapidity correlations between protons and antiprotons. Such correlations originate from the early phase of the collision. The experimental results are compared with HIJING and EPOS model calculations, and the dependence of the fluctuation measurements on the phase-space coverage is examined in the context of lattice quantum chromodynamics (LQCD) and hadron resonance gas (HRG) model estimations. The measured third-order cumulants are consistent with zero within experimental uncertainties of about 4% and are described well by LQCD and HRG predictions.
The interaction of K− with protons is characterised by the presence of several coupled channels, systems like K¯¯¯¯0n and πΣ with a similar mass and the same quantum numbers as the K−p state. The strengths of these couplings to the K−p system are of crucial importance for the understanding of the nature of the Λ(1405) resonance and of the attractive K−p strong interaction. In this article, we present measurements of the K−p correlation functions in relative momentum space obtained in pp collisions at s√ = 13 TeV, in p-Pb collisions at sNN−−−√ = 5.02 TeV, and (semi)peripheral Pb-Pb collisions at sNN−−−√ = 5.02 TeV. The emitting source size, composed of a core radius anchored to the K+p correlation and of a resonance halo specific to each particle pair, varies between 1 and 2 fm in these collision systems. The strength and the effects of the K¯¯¯¯0n and πΣ inelastic channels on the measured K−p correlation function are investigated in the different colliding systems by comparing the data with state-of-the-art models of chiral potentials. A novel approach to determine the conversion weights ω, necessary to quantify the amount of produced inelastic channels in the correlation function, is presented. In this method, particle yields are estimated from thermal model predictions, and their kinematic distribution from blast-wave fits to measured data. The comparison of chiral potentials to the measured K−p interaction indicates that, while the πΣ−K−p dynamics is well reproduced by the model, the coupling to the K¯¯¯¯0n channel in the model is currently underestimated.
The measurement of the production of f0(980) in inelastic pp collisions at s√=5.02 TeV is presented. This is the first reported measurement of inclusive f0(980) production at LHC energies. The production is measured at midrapidity, |y|<0.5, in a wide transverse momentum range, 0<pT<16 GeV/c, by reconstructing the resonance in the f0(980)→π+π− hadronic decay channel using the ALICE detector. The pT-differential yields are compared to those of pions, protons and ϕ mesons as well as to predictions from the HERWIG 7.2 QCD-inspired Monte Carlo event generator and calculations from a coalescence model that uses the AMPT model as an input. The ratio of the pT-integrated yield of f0(980) relative to pions is compared to measurements in e+e− and pp collisions at lower energies and predictions from statistical hadronisation models and HERWIG 7.2. A mild collision energy dependence of the f0(980) to pion production is observed in pp collisions from SPS to LHC energies. All considered models underpredict the pT-integrated f0(980)/(π++π−) ratio. The prediction from the γs-CSM model assuming a zero total strangeness content of f0(980) is consistent with the data within 1.9σ and is the closest to the data. The results provide an essential reference for future measurements of the particle yield and nuclear modification in p−Pb and Pb−Pb collisions, which have been proposed to be instrumental to probe the elusive nature and quark composition of the f0(980) scalar meson.
Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at √sNN = 5.02 TeV
(2022)
The first measurements of elliptic flow of π±, K±, p+p¯¯¯, K0S, Λ+Λ¯¯¯¯, ϕ, Ξ−+Ξ+, and Ω−+Ω+ using multiparticle cumulants in Pb−Pb collisions at sNN−−−√ = 5.02 TeV are presented. Results obtained with two- (v2{2}) and four-particle cumulants (v2{4}) are shown as a function of transverse momentum, pT, for various collision centrality intervals. Combining the data for both v2{2} and v2{4} also allows us to report the first measurements of the mean elliptic flow, elliptic flow fluctuations, and relative elliptic flow fluctuations for various hadron species. These observables probe the event-by-event eccentricity fluctuations in the initial state and the contributions from the dynamic evolution of the expanding quark-gluon plasma. The characteristic features observed in previous pT-differential anisotropic flow measurements for identified hadrons with two-particle correlations, namely the mass ordering at low pT and the approximate scaling with the number of constituent quarks at intermediate pT, are similarly present in the four-particle correlations and the combinations of v2{2} and v2{4}. In addition, a particle species dependence of flow fluctuations is observed that could indicate a significant contribution from final state hadronic interactions. The comparison between experimental measurements and CoLBT model calculations, which combine the various physics processes of hydrodynamics, quark coalescence, and jet fragmentation, illustrates their importance over a wide pT range.
The study of the azimuthal anisotropy of inclusive muons produced in p-Pb collisions at sNN−−−√=8.16 TeV, using the ALICE detector at the LHC is reported. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, v2, is performed as a function of transverse momentum pT in the 0-20% high-multiplicity interval at both forward (2.03<yCMS<3.53) and backward (−4.46<yCMS<−2.96) rapidities over a wide pT range, 0.5<pT<10 GeV/c, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at pT>2 GeV/c. The v2 coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward-central two-particle correlations. Both techniques give compatible results. A positive v2 is measured at both forward and backward rapidities with a significance larger than 4.7σ and 7.6σ, respectively, in the interval 2<pT<6 GeV/c. Comparisons with previous measurements in p-Pb collisions at sNN−−−√=5.02 TeV, and with AMPT and CGC-based theoretical calculations are discussed. The findings impose new constraints on the theoretical interpretations of the origin of the collective behaviour in small collision systems.
The study of the azimuthal anisotropy of inclusive muons produced in p-Pb collisions at sNN−−−√=8.16 TeV, using the ALICE detector at the LHC is reported. The measurement of the second-order Fourier coefficient of the particle azimuthal distribution, v2, is performed as a function of transverse momentum pT in the 0-20% high-multiplicity interval at both forward (2.03<yCMS<3.53) and backward (−4.46<yCMS<−2.96) rapidities over a wide pT range, 0.5<pT<10 GeV/c, in which a dominant contribution of muons from heavy-flavour hadron decays is expected at pT>2 GeV/c. The v2 coefficient of inclusive muons is extracted using two different techniques, namely two-particle cumulants, used for the first time for heavy-flavour measurements, and forward-central two-particle correlations. Both techniques give compatible results. A positive v2 is measured at both forward and backward rapidities with a significance larger than 4.7σ and 7.6σ, respectively, in the interval 2<pT<6 GeV/c. Comparisons with previous measurements in p-Pb collisions at sNN−−−√=5.02 TeV, and with AMPT and CGC-based theoretical calculations are discussed. The findings impose new constraints on the theoretical interpretations of the origin of the collective behaviour in small collision systems.
In ultraperipheral collisions (UPCs) of relativistic nuclei without overlap of nuclear densities, the two nuclei are excited by the Lorentz-contracted Coulomb fields of their collision partners. In these UPCs, the typical nuclear excitation energy is below a few tens of MeV, and a small number of nucleons are emitted in electromagnetic dissociation (EMD) of primary nuclei, in contrast to complete nuclear fragmentation in hadronic interactions. The cross sections of emission of given numbers of neutrons in UPCs of 208Pb nuclei at sNN−−−√=5.02 TeV were measured with the neutron zero degree calorimeters (ZDCs) of the ALICE detector at the LHC, exploiting a similar technique to that used in previous studies performed at sNN−−−√=2.76 TeV. In addition, the cross sections for the exclusive emission of one, two, three, four, and five forward neutrons in the EMD, not accompanied by the emission of forward protons, and thus mostly corresponding to the production of 207,206,205,204,203Pb, respectively, were measured for the first time. The predictions from the available models describe the measured cross sections well. These cross sections can be used for evaluating the impact of secondary nuclei on the LHC components, in particular, on superconducting magnets, and also provide useful input for the design of the Future Circular Collider (FCC-hh).
W±-boson production in p–Pb collisions at √sNN = 8.16 TeV and Pb–Pb collisions at √sNN = 5.02 TeV
(2022)
The production of the W± bosons measured in p−Pb collisions at a centre-of-mass energy per nucleon−nucleon collision sNN−−−−√=8.16 TeV and Pb−Pb collisions at sNN−−−−√=5.02 TeV with ALICE at the LHC is presented. The W± bosons are measured via their muonic decay channel, with the muon reconstructed in the pseudorapidity region −4<ημlab<−2.5 with transverse momentum pμT>10 GeV/c. While in Pb−Pb collisions the measurements are performed in the forward (2.5<yμcms<4) rapidity region, in p−Pb collisions, where the centre-of-mass frame is boosted with respect to the laboratory frame, the measurements are performed in the backward (−4.46<yμcms<−2.96) and forward (2.03<yμcms<3.53) rapidity regions. The W− and W+ production cross sections, lepton-charge asymmetry, and nuclear modification factors are evaluated as a function of the muon rapidity. In order to study the production as a function of the p−Pb collision centrality, the production cross sections of the W− and W+ bosons are combined and normalised to the average number of binary nucleon−nucleon collision ⟨Ncoll⟩. In Pb−Pb collisions, the same measurements are presented as a function of the collision centrality. Study of the binary scaling of the W±-boson cross sections in p−Pb and Pb−Pb collisions is also reported. The results are compared with perturbative QCD (pQCD) calculations, with and without nuclear modifications of the Parton Distribution Functions (PDFs), as well as with available data at the LHC. Significant deviations from the theory expectations are found in the two collision systems, indicating that the measurements can provide additional constraints for the determination of nuclear PDF (nPDFs) and in particular of the light-quark distributions.
W±-boson production in p–Pb collisions at √sNN = 8.16 TeV and Pb–Pb collisions at √sNN = 5.02 TeV
(2022)
The production of the W± bosons measured in p−Pb collisions at a centre-of-mass energy per nucleon−nucleon collision sNN−−−−√=8.16 TeV and Pb−Pb collisions at sNN−−−−√=5.02 TeV with ALICE at the LHC is presented. The W± bosons are measured via their muonic decay channel, with the muon reconstructed in the pseudorapidity region −4<ημlab<−2.5 with transverse momentum pμT>10 GeV/c. While in Pb−Pb collisions the measurements are performed in the forward (2.5<yμcms<4) rapidity region, in p−Pb collisions, where the centre-of-mass frame is boosted with respect to the laboratory frame, the measurements are performed in the backward (−4.46<yμcms<−2.96) and forward (2.03<yμcms<3.53) rapidity regions. The W− and W+ production cross sections, lepton-charge asymmetry, and nuclear modification factors are evaluated as a function of the muon rapidity. In order to study the production as a function of the p−Pb collision centrality, the production cross sections of the W− and W+ bosons are combined and normalised to the average number of binary nucleon−nucleon collision ⟨Ncoll⟩. In Pb−Pb collisions, the same measurements are presented as a function of the collision centrality. Study of the binary scaling of the W±-boson cross sections in p−Pb and Pb−Pb collisions is also reported. The results are compared with perturbative QCD (pQCD) calculations, with and without nuclear modifications of the Parton Distribution Functions (PDFs), as well as with available data at the LHC. Significant deviations from the theory expectations are found in the two collision systems, indicating that the measurements can provide additional constraints for the determination of nuclear PDF (nPDFs) and in particular of the light-quark distributions.
The production of electrons from heavy-flavour hadron decays was measured as a function of transverse momentum (pT) in minimum-bias p–Pb collisions at sNN=5.02 TeV using the ALICE detector at the LHC. The measurement covers the pT interval 0.5<pT<12 GeV/c and the rapidity range −1.065<ycms<0.135 in the centre-of-mass reference frame. The contribution of electrons from background sources was subtracted using an invariant mass approach. The nuclear modification factor RpPb was calculated by comparing the pT-differential invariant cross section in p–Pb collisions to a pp reference at the same centre-of-mass energy, which was obtained by interpolating measurements at s=2.76 TeV and s=7 TeV. The RpPb is consistent with unity within uncertainties of about 25%, which become larger for pT below 1 GeV/c. The measurement shows that heavy-flavour production is consistent with binary scaling, so that a suppression in the high-pT yield in Pb–Pb collisions has to be attributed to effects induced by the hot medium produced in the final state. The data in p–Pb collisions are described by recent model calculations that include cold nuclear matter effects.
Inclusive photon production at forward rapidities in pp and p–Pb
collisions at √sNN = 5.02 TeV
(2023)
A study of multiplicity and pseudorapidity distributions of inclusive photons measured in pp and p−Pb collisions at a center-of-mass energy per nucleon−nucleon collision of sNN−−−√=5.02 TeV using the ALICE detector in the forward pseudorapidity region 2.3<ηlab<3.9 is presented. Measurements in p−Pb collisions are reported for two beam configurations in which the directions of the proton and lead ion beam were reversed. The pseudorapidity distributions in p−Pb collisions are obtained for seven centrality classes which are defined based on different event activity estimators, i.e., the charged-particle multiplicity measured at midrapidity as well as the energy deposited in a calorimeter at beam rapidity. The inclusive photon multiplicity distributions for both pp and p−Pb collisions are described by double negative binomial distributions. The pseudorapidity distributions of inclusive photons are compared to those of charged particles at midrapidity in \pp collisions and for different centrality classes in p−Pb collisions. The results are compared to predictions from various Monte Carlo event generators. None of the generators considered in this paper reproduces the inclusive photon multiplicity distributions in the reported multiplicity range. The pseudorapidity distributions are, however, better described by the same generators.
The transverse-momentum (pT) spectra and coalescence parameters B2 of (anti)deuterons are measured in pp collisions at s√=13 TeV in and out of jets. In this measurement, the direction of the leading particle with the highest pT in the event (pleadT>5 GeV/c) is used as an approximation for the jet axis. The event is consequently divided into three azimuthal regions and the jet signal is obtained as the difference between the Toward region, that contains jet fragmentation products in addition to the underlying event (UE), and the Transverse region, which is dominated by the UE. The coalescence parameter in the jet is found to be approximately a factor of 10 larger than that in the underlying event. This experimental observation is consistent with the coalescence picture and can be attributed to the smaller average phase-space distance between nucleons inside the jet cone as compared to the underlying event. The results presented in this Letter are compared to predictions from a simple nucleon coalescence model, where the phase space distributions of nucleons are generated using PYTHIA 8 with the Monash 2013 tuning, and to predictions from a deuteron production model based on ordinary nuclear reactions with parametrized energy-dependent cross sections tuned on data. The latter model is implemented in PYTHIA 8.3. Both models reproduce the observed large difference between in-jet and out-of-jet coalescence parameters.
A new, more precise measurement of the Λ hyperon lifetime is performed using a large data sample of Pb−Pb collisions at sNN−−−√=5.02 TeV with ALICE. The Λ and Λ¯¯¯¯ hyperons are reconstructed at midrapidity using their two-body weak decay channel Λ→p+π− and Λ¯¯¯¯→p¯¯¯+π+. The measured value of the Λ lifetime is τΛ=[261.07±0.37 (stat.)±0.72 (syst.)] ps. The relative difference between the lifetime of Λ and Λ¯¯¯¯, which represents an important test of CPT invariance in the strangeness sector, is also measured. The obtained value (τΛ−τΛ¯¯¯¯)/τΛ=0.0013±0.0028 (stat.)±0.0021 (syst.) is consistent with zero within the uncertainties. Both measurements of the Λ hyperon lifetime and of the relative difference between τΛ and τΛ¯¯¯¯ are in agreement with the corresponding world averages of the Particle Data Group and about a factor of three more precise.
Multiplicity (Nch) distributions and transverse momentum (pT) spectra of inclusive primary charged particles in the kinematic range of |η|<0.8 and 0.15GeV/c<pT<10GeV/c are reported for pp, p-Pb, Xe-Xe and Pb-Pb collisions at centre-of-mass energies per nucleon pair ranging from sNN−−−√=2.76 TeV up to 13 TeV. A sequential two-dimensional unfolding procedure is used to extract the correlation between the transverse momentum of primary charged particles and the charged-particle multiplicity of the corresponding collision. This correlation sharply characterises important features of the final state of a collision and, therefore, can be used as a stringent test of theoretical models. The multiplicity distributions as well as the mean and standard deviation derived from the pT spectra are compared to state-of-the-art model predictions.
This letter reports the first measurement of spin alignment, with respect to the helicity axis, for D∗+ vector mesons and their charge conjugates from charm-quark hadronisation (prompt) and from beauty-meson decays (non-prompt) in hadron collisions. The measurements were performed at midrapidity (|y|<0.8) as a function of transverse momentum (pT) in proton-proton (pp) collisions collected by ALICE at the centre-of-mass energy s√=13 TeV. The diagonal spin density matrix element ρ00 of D∗+ mesons was measured from the angular distribution of the D∗+→D0(→K−π+)π+ decay products, in the D∗+ rest frame, with respect to the D∗+ momentum direction in the pp centre of mass frame. The ρ00 value for prompt D∗+ mesons is consistent with 1/3, which implies no spin alignment. However, for non-prompt D∗+ mesons an evidence of ρ00 larger than 1/3 is found. The measured value of the spin density element is ρ00=0.455±0.022(stat.)±0.035(syst.) in the 5<pT<20 GeV/c interval, which is consistent with a PYTHIA 8 Monte Carlo simulation coupled with the EVTGEN package, which implements the helicity conservation in the decay of D∗+ meson from beauty mesons. In non-central heavy-ion collisions, the spin of the D∗+ mesons may be globally aligned with the direction of the initial angular momentum and magnetic field. Based on the results for pp collisions reported in this letter it is shown that alignment of non-prompt D∗+ mesons due to the helicity conservation coupled to the collective anisotropic expansion may mimic the signal of global spin alignment in heavy-ion collisions.
An excess of J/ψ yield at very low transverse momentum (pT<0.3 GeV/c), originating from coherent photoproduction, is observed in peripheral and semicentral hadronic Pb−Pb collisions at a center-of-mass energy per nucleon pair of √sNN=5.02 TeV. The measurement is performed with the ALICE detector via the dimuon decay channel at forward rapidity (2.5<y<4). The nuclear modification factor at very low pT and the coherent photoproduction cross section are measured as a function of centrality down to the 10% most central collisions. These results extend the previous study at √sNN=2.76 TeV, confirming the clear excess over hadronic production in the pT range 0−0.3 GeV/c and the centrality range 70−90%, and establishing an excess with a significance greater than 5σ also in the 50−70% and 30−50% centrality ranges. The results are compared with earlier measurements at √sNN=2.76 TeV and with different theoretical predictions aiming at describing how coherent photoproduction occurs in hadronic interactions with nuclear overlap.
The production of inclusive, prompt and non-prompt J/ψ was studied for the first time at midrapidity (−1.37<ycms<0.43) in p−Pb collisions at sNN−−−√=8.16 TeV with the ALICE detector at the LHC. The inclusive J/ψ mesons were reconstructed in the dielectron decay channel in the transverse momentum (pT) interval 0<pT<14 GeV/c and the prompt and non-prompt contributions were separated on a statistical basis for pT>2 GeV/c. The study of the J/ψ mesons in the dielectron channel used for the first time in ALICE online single-electron triggers from the Transition Radiation Detector, providing a data sample corresponding to an integrated luminosity of 689±13μb−1. The proton−proton reference cross section for inclusive J/ψ was obtained based on interpolations of measured data at different centre-of-mass energies and a universal function describing the pT-differential J/ψ production cross sections. The pT-differential nuclear modification factors RpPb of inclusive, prompt, and non-prompt J/ψ are consistent with unity and described by theoretical models implementing only nuclear shadowing.
The production of π±, K±, and (p¯¯¯)p is measured in pp collisions at s√=13 TeV in different topological regions. Particle transverse momentum (pT) spectra are measured in the ``toward'', ``transverse'', and ``away'' angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT=NT/⟨NT⟩, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and ⟨NT⟩ is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. The yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. The pT-differential particle ratios (p+p¯¯¯)/(π++π−) and (K++K−)/(π++π−) in the low UE limit (RT→0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.
The STAR experiment at RHIC reports new measurements of jet quenching based on the semi-inclusive distribution of charged-particle jets recoiling from direct photon (γdir) and neutral pion (π0) triggers in p+p and central Au+Au collisions at √sNN=200 GeV, for triggers in the range 9<EtrigT<20 GeV. The datasets have integrated luminosities of 3.9 nb−1 for Au+Au and 23 pb−1 for p+p collisions. Jets are reconstructed using the anti-kT algorithm with resolution parameters R=0.2 and 0.5. The large uncorrelated jet background in central Au+Au collisions is corrected using a mixed-event approach, which enables precise charged-particle jet measurements at low transverse momentum pchT,jet and large R. Recoil-jet distributions are reported in the range pchT,jet<25 GeV. Comparison of the distributions measured in p+p and Au+Au collisions reveals strong medium-induced jet yield suppression for R=0.2, with markedly less suppression for R=0.5. These data provide new insight into the mechanisms underlying jet quenching, and the angular dependence of medium-induced jet-energy transport.
The differential cross section for Z0 production, measured as a function of the boson's transverse momentum (pT), provides important constraints on the evolution of the transverse momentum dependent parton distribution functions (TMDs). The transverse single spin asymmetry (TSSA) of the Z0 is sensitive to one of the polarized TMDs, the Sivers function, which is predicted to have the opposite sign in p+p →W/Z+X from that which enters in semi-inclusive deep inelastic scattering. In this Letter, the STAR Collaboration reports the first measurement of the Z0/γ∗ differential cross section as a function of its pT in p+p collisions at a center-of-mass energy of 510 GeV, together with the Z0/γ∗ total cross section. We also report the measurement of Z0/γ∗ TSSA in transversely polarized p+p collisions at 510 GeV.
Measurements of mass and Λ binding energy of 4ΛH and 4ΛHe in Au+Au collisions at √sNN=3 GeV are presented, with an aim to address the charge symmetry breaking (CSB) problem in hypernuclei systems with atomic number A = 4. The Λ binding energies are measured to be 2.22±0.06(stat.)±0.14(syst.) MeV and 2.38±0.13(stat.)±0.12(syst.) MeV for 4ΛH and 4ΛHe, respectively. The measured Λ binding-energy difference is 0.16±0.14(stat.)±0.10(syst.) MeV for ground states. Combined with the γ-ray transition energies, the binding-energy difference for excited states is −0.16±0.14(stat.)±0.10(syst.) MeV, which is negative and comparable to the value of the ground states within uncertainties. These new measurements on the Λ binding-energy difference in A = 4 hypernuclei systems are consistent with the theoretical calculations that result in ΔB4Λ(1+exc) ≈ −ΔB4Λ(0+g.s.)<0 and present a new method for the study of CSB effect using relativistic heavy-ion collisions.
In relativistic heavy-ion collisions, a global spin polarization, PH, of Λ and Λ¯ hyperons along the direction of the system angular momentum was discovered and measured across a broad range of collision energies and demonstrated a trend of increasing PH with decreasing sNN−−−√. A splitting between Λ and Λ¯ polarization may be possible due to their different magnetic moments in a late-stage magnetic field sustained by the quark-gluon plasma which is formed in the collision. The results presented in this study find no significant splitting at the collision energies of sNN−−−√=19.6 and 27 GeV in the RHIC Beam Energy Scan Phase II using the STAR detector, with an upper limit of PΛ¯−PΛ<0.24% and PΛ¯−PΛ<0.35%, respectively, at a 95% confidence level. We derive an upper limit on the naïve extraction of the late-stage magnetic field of B<9.4⋅1012 T and B<1.4⋅1013 T at sNN−−−√=19.6 and 27 GeV, respectively, although more thorough derivations are needed. Differential measurements of PH were performed with respect to collision centrality, transverse momentum, and rapidity. With our current acceptance of |y|<1 and uncertainties, we observe no dependence on transverse momentum and rapidity in this analysis. These results challenge multiple existing model calculations following a variety of different assumptions which have each predicted a strong dependence on rapidity in this collision-energy range.
We present the first measurements of transverse momentum spectra of π±, K±, p(p¯) at midrapidity (|y|<0.1) in U+U collisions at sNN−−−−√ = 193 GeV with the STAR detector at the Relativistic Heavy Ion Collider (RHIC). The centrality dependence of particle yields, average transverse momenta, particle ratios and kinetic freeze-out parameters are discussed. The results are compared with the published results from Au+Au collisions at \snn = 200 GeV in STAR. The results are also compared to those from A Multi Phase Transport (AMPT) model.
We report the beam energy and collision centrality dependence of fifth and sixth order cumulants (C5, C6) and factorial cumulants (κ5, κ6) of net-proton and proton distributions, from sNN−−−−√=3−200 GeV Au+Au collisions at RHIC. The net-proton cumulant ratios generally follow the hierarchy expected from QCD thermodynamics, except for the case of collisions at sNN−−−−√ = 3 GeV. C6/C2 for 0-40\% centrality collisions is increasingly negative with decreasing sNN−−−−√, while it is positive for the lowest sNN−−−−√ studied. These observed negative signs are consistent with QCD calculations (at baryon chemical potential, μB≤ 110 MeV) that include a crossover quark-hadron transition. In addition, for sNN−−−−√≥ 11.5 GeV, the measured proton κn, within uncertainties, does not support the two-component shape of proton distributions that would be expected from a first-order phase transition. Taken in combination, the hyper-order proton number fluctuations suggest that the structure of QCD matter at high baryon density, μB∼750 MeV (sNN−−−−√ = 3 GeV) is starkly different from those at vanishing μB∼20MeV (sNN−−−−√ = 200 GeV and higher).
We report a measurement of cumulants and correlation functions of event-by-event proton multiplicity distributions from fixed-target Au+Au collisions at sNN−−−√ = 3 GeV measured by the STAR experiment. Protons are identified within the rapidity (y) and transverse momentum (pT) region −0.9<y<0 and 0.4<pT<2.0 GeV/c in the center-of-mass frame. A systematic analysis of the proton cumulants and correlation functions up to sixth-order as well as the corresponding ratios as a function of the collision centrality, pT, and y are presented. The effect of pileup and initial volume fluctuations on these observables and the respective corrections are discussed in detail. The results are compared to calculations from the hadronic transport UrQMD model as well as a hydrodynamic model. In the most central 5\% collisions, the value of proton cumulant ratio C4/C2 is negative, drastically different from the values observed in Au+Au collisions at higher energies. Compared to model calculations including Lattice QCD, a hadronic transport model, and a hydrodynamic model, the strong suppression in the ratio of C4/C2 at 3 GeV Au+Au collisions indicates an energy regime dominated by hadronic interactions.
We report on measurements of sequential Υ suppression in Au+Au collisions at √sNN = 200 GeV with the STAR detector at the Relativistic Heavy Ion Collider (RHIC) through both the di-electron and di-muon channels. In the 0-60% centrality class, the nuclear modification factors (RAA), which quantify the level of yield suppression in heavy-ion collisions compared to p+p collisions, for Υ(1S) and Υ(2S) are 0.40±0.03 (stat.)±0.03 (sys.)±0.07 (norm.) and 0.26±0.07 (stat.)±0.02 (sys.)±0.04 (norm.), respectively, while the upper limit of the Υ(3S) RAA is 0.20 at a 95% confidence level. This observation provides experimental evidence that the Υ(3S) is significantly more suppressed than the Υ(1S) at RHIC. The level of suppression for Υ(1S) is comparable to that observed at the much higher collision energy at the Large Hadron Collider. These results point to the creation of a deconfined medium at RHIC whose temperature is sufficiently high to strongly suppress excited Υ states.
We report the triton (t) production in Au+Au collisions at sNN−−−√ = 7.7 -- 200 GeV measured at mid-rapidity (|y|< 0.5) by the STAR experiment from the first phase of the beam energy scan at the Relativistic Heavy Ion Collider (RHIC). The nuclear compound yield ratio (Nt×Np/N2d), which is predicted to be sensitive to the local density fluctuation of neutrons, monotonically decreases with increasing charged-particle multiplicity (dNch/dη) and exhibits a scaling behavior. The multiplicity dependence of the yield ratios are compared with calculations from coalescence and thermal models. Relative to the coalescence baseline, enhancements of the yield ratios are observed in the 0%-10% most central collisions at 19.6 and 27 GeV with a significance of 2.3σ and 3.4σ, respectively, with a combined significance of 4.1σ. The measured significance of these enhancements decreases with smaller pT acceptance. The enhancements are not observed in peripheral collisions and model calculations without critical fluctuation. Important implications on the QCD phase structure and the production mechanism of light nuclei in heavy-ion collisions are discussed.
Atomic nuclei are self-organized, many-body quantum systems bound by strong nuclear forces within femtometer-scale space. These complex systems manifest a diverse set of shapes~, traditionally explored via non-invasive spectroscopic techniques at low energies. Their instantaneous shapes, obscured by long-timescale quantum fluctuations, are considered not directly observable at low energy. We introduce a complementary method, collective flow assisted nuclear shape imaging, to image the nuclear global shape by colliding them at ultrarelativistic speeds and analyzing the collective response of outgoing debris. This technique captures a collision-specific snapshot of the spatial matter distribution in the nuclei, which, through the hydrodynamic expansion, leaves imprints on the particle momentum distribution patterns observed in detectors. We benchmark this method in collisions of ground state Uranium-238 nuclei, known for its elongated, axial-symmetric shape. Our findings, while confirming an overall deformation broadly consistent with prior low-energy experiments, also indicate a small deviation from axial symmetry in the nuclear ground state. This approach marks a new way of imaging nuclei, especially those with uncertain shape characteristics, and refines initial conditions in high-energy nuclear collisions. It tackles the important issue of nuclear structure evolution across various energy scales.
Flow coefficients (v2 and v3) are measured in high-multiplicity p+Au, d+Au, and 3He+Au collisions at a center-of-mass energy of √sNN = 200 GeV using the STAR detector. The measurements are conducted using two-particle correlations with a pseudorapidity requirement of |η|< 0.9 and a pair gap of |Δη|>1.0. The primary focus of this paper is on the analysis procedures and methods employed, especially the subtraction of non-flow contributions. Four well-established non-flow subtraction methods are applied to determine vn, and their validity is verified using the HIJING event generator. The vn values are compared across the three collision systems at similar multiplicities, which allows for cancellation of final state effects and isolation of the impact of the initial geometry. While the v2 values display differences among these collision systems, the v3 values are largely similar, consistent with the expectations of subnucleon fluctuations in the initial geometry. The ordering of vn differs quantitatively from previous measurements obtained using two-particle correlations with a larger rapidity gap; this difference could be partially attributed to the effects of flow decorrelations in the rapidity direction.
We measure triangular flow relative to the reaction plane at 3 GeV center-of-mass energy in Au+Au collisions at RHIC. A significant v3 signal is observed for protons, whose magnitude increases for higher rapidity, higher transverse momentum, and more peripheral collisions. The triangular flow is essentially rapidity-odd with a rapidity slope at mid-rapidity, dv3/dy|(y=0), opposite in sign compared to the slope for directed flow. No significant v3 signal is observed for charged pions and kaons. Comparisons with models suggest that a mean field potential is required to describe these results, and that the triangular shape of the participant nucleons is the result of stopping and nuclear geometry.
We report here the first observation of directed flow (v1) of the hypernuclei 3ΛH and 4ΛH in mid-central Au+Au collisions at sNN−−−√ = 3 GeV at RHIC. These data are taken as part of the beam energy scan program carried out by the STAR experiment. From 165 million good events in 5-40% centrality, about 8400 3ΛH and 5200 4ΛH candidates are reconstructed through two- and three-body decay channels. We observe that these hypernuclei exhibit significant directed flow. Comparing to that of light nuclei, it is found that the mid-rapidity v1 slopes of 3ΛH and 4ΛH follow baryon number scaling, implying that the coalescence is the dominant mechanism for these hypernuclei production in such collisions.
We report the differential yields at mid-rapidity of the Breit-Wheeler process (γγ→e+e−) in peripheral Au+Au collisions at sNN−−−√= 54.4 GeV and 200 GeV with the STAR experiment at RHIC, as a function of energy sNN−−−√, e+e− transverse momentum pT, p2T, invariant mass Mee and azimuthal angle. In the invariant mass range of 0.4 < Mee < 2.6 GeV/c2 at low transverse momentum (pT <0.15 GeV/c), the yields increase while the pair ⟨p2T⟩−−−−√ decreases with increasing sNN−−−√, a feature is correctly predicted by the QED calculation. The energy dependencies of the measured quantities are sensitive to the nuclear form factor, infrared divergence and photon polarization. The data are compiled and used to extract the charge radius of the Au nucleus.
We report directed flow (v1) of multistrange baryons (Ξ and Ω) and improved v1 data for K−, p¯, Λ¯ and ϕ in Au+Au collisions at sNN−−−√=27 and 200 GeV from the STAR at the Relativistic Heavy Ion Collider (RHIC). We focus on particles whose constituent quarks are not transported from beam rapidity rather produced in the collisions. In midcentral collisions, we observe a coalescence sum rule for hadron combinations with identical quark content and a difference (``splitting'') in the slope of v1 vs. rapidity for combinations having nonidentical quark content. The splitting strength appears to increase with the electric charge difference and strangeness content difference of the constituent quarks in the combinations, consistent with an electromagnetic effect. The peripheral collision statistics are insufficient to draw firm conclusions.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2023)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane. This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions. A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of \(R=0.4\) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb+Pb collision data.
Jet-hadron correlations with respect to the event plane in √sNN = 200 GeV Au+Au collisions in STAR
(2023)
Angular distributions of charged particles relative to jet axes are studied in sNN−−−√ = 200 GeV Au+Au collisions as a function of the jet orientation with respect to the event plane.This differential study tests the expected path-length dependence of energy loss experienced by a hard-scattered parton as it traverses the hot and dense medium formed in heavy-ion collisions.A second-order event plane is used in the analysis as an experimental estimate of the reaction plane formed by the collision impact parameter and the beam direction. Charged-particle jets with 15<pT,jet< 20 and 20<pT,jet< 40 GeV/c were reconstructed with the anti-kT algorithm with radius parameter setting of \(R=0.4\) in the 20-50\% centrality bin to maximize the initial-state eccentricity of the interaction region. The reaction plane fit method is implemented to remove the flow-modulated background with better precision than prior methods. Yields and widths of jet-associated charged-hadron distributions are extracted in three angular bins between the jet axis and the event plane. The event-plane (EP) dependence is further quantified by ratios of the associated yields in different EP bins. No dependence on orientation of the jet axis with respect to the event plane is seen within the uncertainties in the kinematic regime studied. This finding is consistent with a similar experimental observation by ALICE in sNN−−−√ = 2.76 TeV Pb-Pb collision data.
We report a new measurement of transverse single-spin asymmetries for dijet production in collisions of polarized protons at s√ = 200 GeV. Correlations between the proton spin and the transverse momenta of its partons, each perpendicular to the proton momentum direction, are probed at high Q2 ≈160 GeV2. The associated Sivers observable ⟨kT⟩, the average parton transverse momentum, is extracted using simple kinematics. Nonzero Sivers effects are observed for the first time in dijets from proton-proton collisions, but only when the jets are sorted by their net charge, which enhances the u- or d-quark contributions to separate data samples. This also enables a simple kinematic approach for determination of the individual partonic contributions to the observed asymmetries.
We report a new measurement of transverse single-spin asymmetries for dijet production in collisions of polarized protons at s√ = 200 GeV. Possible correlations between the proton spin and the transverse momenta of its partons, mutually orthogonal, with each perpendicular to the proton momentum direction, are probed at high Q2 ≈160 GeV2. The associated Sivers observable ⟨kT⟩, the average parton transverse momentum, is extracted using simple kinematics. Nonzero Sivers effects are observed for the first time in proton-proton collisions, but only when the jets are sorted by their net charge, which enhances the u- or d-quark contributions to separate data samples. This also enables a determination of the individual partonic contributions to the observed asymmetries.
We report the first measurements of cumulants, up to 4th order, of deuteron number distributions and proton-deuteron correlations in Au+Au collisions recorded by the STAR experiment in phase-I of Beam Energy Scan (BES-I) program at the Relativistic Heavy Ion Collider (RHIC). Deuteron cumulants, their ratios, and proton-deuteron mixed cumulants are presented for different collision centralities covering a range of center of mass energy per nucleon pair sNN−−−√ = 7.7 to 200 GeV. It is found that the cumulant ratios at lower collision energies favor a canonical ensemble over a grand canonical ensemble in thermal models. An anti-correlation between proton and deuteron multiplicity is observed across all collision energies and centralities, consistent with the expectation from global baryon number conservation. The UrQMD model coupled with a phase-space coalescence mechanism qualitatively reproduces the collision-energy dependence of cumulant ratios and proton-deuteron correlations.
We report multi-differential measurements of strange hadron production ranging from mid- to target-rapidity in Au+Au collisions at a center-of-momentum energy per nucleon pair of sNN−−−√=3 GeV with the STAR experiment at RHIC. K0S meson and Λ hyperon yields are measured via their weak decay channels. Collision centrality and rapidity dependences of the transverse momentum spectra and particle ratios are presented. Particle mass and centrality dependence of the average transverse momenta of Λ and K0S are compared with other strange particles, providing evidence of the development of hadronic rescattering in such collisions. The 4π yields of each of these strange hadrons show a consistent centrality dependence. Discussions on radial flow, the strange hadron production mechanism, and properties of the medium created in such collisions are presented together with results from hadronic transport and thermal model calculations.
Antimatter is a research topic of fundamental interest. Sufficient matter-antimatter asymmetry in the early Universe created the matter-dominated world today. The origin of this asymmetry is not completely understood to date. High-energy nuclear collisions create conditions similar to the Universe microseconds after the Big Bang, with comparable amounts of matter and antimatter. Much of the antimatter created escapes the rapidly expanding fireball without annihilation, making such collisions an effective experimental tool to create heavy antimatter nuclear objects and study their properties. In this paper, we report the first observation of the antimatter hypernucleus 4Λ¯H¯¯¯¯, composed of an Λ¯, an antiproton and two antineutrons. The discovery was made through its two-body decay after production in ultrarelativistic heavy-ion collisions by the STAR experiment at the Relativistic Heavy Ion Collider. In total, 15.6 candidate 4Λ¯H¯¯¯¯ antimatter hypernuclei are obtained with an estimated background count of 6.4. Lifetimes of the antihypernuclei 3Λ¯H¯¯¯¯ and 4Λ¯H¯¯¯¯ are measured and compared with the lifetimes of their corresponding hypernuclei, testing the symmetry between matter and antimatter. Various production yield ratios among (anti)hypernuclei and (anti)nuclei are also measured and compared with theoretical model predictions, shedding light on their production mechanism.
In heavy-ion collision experiments, the global collectivity of final-state particles can be quantified by anisotropic flow coefficients (vn). The first-order flow coefficient, also referred to as the directed flow (v1), describes the collective sideward motion of produced particles and nuclear fragments in heavy-ion collisions. It carries information on the very early stage of the collision, especially at large pseudorapidity (η), where it is believed to be generated during the nuclear passage time. Directed flow therefore probes the onset of bulk collective dynamics during thermalization, providing valuable experimental guidance to models of the pre-equilibrium stage. In 2018, the Event Plane Detector (EPD) was installed in STAR and used for the Beam Energy Scan phase-II (BES-II) data taking. The combination of EPD (2.1<|η|<5.1) and high-statistics BES-II data enables us to extend the v1 measurement to the forward and backward η regions. In this paper, we present the measurement of v1 over a wide η range in Au+Au collisions at √sNN= 19.6 and 27 GeV using the STAR EPD. The results of the analysis at √sNN=19.6 GeV exhibit excellent consistency with the previous PHOBOS measurement, while elevating the precision of the overall measurement. The increased precision of the measurement also revealed finer structures in heavy-ion collisions, including a potential observation of the first-order event-plane decorrelation. Multiple physics models were compared to the experimental results. Only a transport model and a three-fluid hybrid model can reproduce a sizable v1 at large η as was observed experimentally. The model comparison also indicates v1 at large η might be sensitive to the QGP phase transition.
The longitudinal and transverse spin transfers to Λ (Λ¯¯¯¯) hyperons in polarized proton-proton collisions are expected to be sensitive to the helicity and transversity distributions, respectively, of (anti-)strange quarks in the proton, and to the corresponding polarized fragmentation functions. We report improved measurements of the longitudinal spin transfer coefficient, DLL, and the transverse spin transfer coefficient, DTT, to Λ and Λ¯¯¯¯ in polarized proton-proton collisions at √s = 200 GeV by the STAR experiment at RHIC. The data set includes longitudinally polarized proton-proton collisions with an integrated luminosity of 52 pb−1, and transversely polarized proton-proton collisions with a similar integrated luminosity. Both data sets have about twice the statistics of previous results and cover a kinematic range of |ηΛ(Λ¯¯¯¯)| < 1.2 and transverse momentum pT,Λ(Λ¯¯¯¯) up to 8 GeV/c. We also report the first measurements of the hyperon spin transfer coefficients DLL and DTT as a function of the fractional jet momentum z carried by the hyperon, which can provide more direct constraints on the polarized fragmentation functions.
Elliptic flow of heavy-flavor decay electrons in Au+Au collisions at √sNN = 27 and 54.4 GeV at RHIC
(2023)
We report on new measurements of elliptic flow (v2) of electrons from heavy-flavor hadron decays at mid-rapidity (|y|<0.8) in Au+Au collisions at sNN−−−√ = 27 and 54.4 GeV from the STAR experiment. Heavy-flavor decay electrons (eHF) in Au+Au collisions at sNN−−−√ = 54.4 GeV exhibit a non-zero v2 in the transverse momentum (pT) region of pT< 2 GeV/c with the magnitude comparable to that at sNN−−−√=200 GeV. The measured eHF v2 at 54.4 GeV is also consistent with the expectation of their parent charm hadron v2 following number-of-constituent-quark scaling as other light and strange flavor hadrons at this energy. These suggest that charm quarks gain significant collectivity through the evolution of the QCD medium and may reach local thermal equilibrium in Au+Au collisions at sNN−−−√=54.4 GeV. The measured eHF v2 in Au+Au collisions at sNN−−−√= 27 GeV is consistent with zero within large uncertainties. The energy dependence of v2 for different flavor particles (π,ϕ,D0/eHF) shows an indication of quark mass hierarchy in reaching thermalization in high-energy nuclear collisions.
Production of protons and light nuclei in Au+Au collisions at √sNN = 3 GeV with the STAR detector
(2023)
We report the systematic measurement of protons and light nuclei production in Au+Au collisions at √sNN = 3 GeV by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The transverse momentum (pT) spectra of protons (p), deuterons (d), tritons (t), 3He, and 4He are measured from mid-rapidity to target rapidity for different collision centralities. We present the rapidity and centrality dependence of particle yields (dN/dy), average transverse momentum (⟨pT⟩), yield ratios (d/p, t/p,3He/p, 4He/p), as well as the coalescence parameters (B2, B3). The 4π yields for various particles are determined by utilizing the measured rapidity distributions, dN/dy. Furthermore, we present the energy, centrality, and rapidity dependence of the compound yield ratios (Np×Nt/N2d) and compare them with various model calculations. The physics implications of those results on the production mechanism of light nuclei and on QCD phase structure are discussed.
The linear and mode-coupled contributions to higher-order anisotropic flow are presented for Au+Au collisions at sNN−−−√ = 27, 39, 54.4, and 200 GeV and compared to similar measurements for Pb+Pb collisions at the Large Hadron Collider (LHC). The coefficients and the flow harmonics' correlations, which characterize the linear and mode-coupled response to the lower-order anisotropies, indicate a beam energy dependence consistent with an influence from the specific shear viscosity (η/s). In contrast, the dimensionless coefficients, mode-coupled response coefficients, and normalized symmetric cumulants are approximately beam-energy independent, consistent with a significant role from initial-state effects. These measurements could provide unique supplemental constraints to (i) distinguish between different initial-state models and (ii) delineate the temperature (T) and baryon chemical potential (μB) dependence of the specific shear viscosity ηs(T,μB).
The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon γdir and neutral-pion (π0) triggers in p+p and central Au+Au collisions at sNN−−−√=200 GeV over a broad kinematic range, for jet resolution parameters R=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The magnitude of suppression is similar for γdir- and π0-triggered data, which constrains the color-charge and path-length dependence of jet quenching. Theoretical model calculations incorporating jet quenching do not fully describe the measurements.
Azimuthal anisotropy measurement of (multi-)strange hadrons in Au+Au collisions at √sNN = 54.4 GeV
(2022)
Azimuthal anisotropy of produced particles is one of the most important observables used to access the collective properties of the expanding medium created in relativistic heavy-ion collisions. In this paper, we present second (v2) and third (v3) order azimuthal anisotropies of K0S, ϕ, Λ, Ξ and Ω at mid-rapidity (|y|<1) in Au+Au collisions at sNN−−−√ = 54.4 GeV measured by the STAR detector. The v2 and v3 are measured as a function of transverse momentum and centrality. Their energy dependence is also studied. v3 is found to be more sensitive to the change in the center-of-mass energy than v2. Scaling by constituent quark number is found to hold for v2 within 10%. This observation could be evidence for the development of partonic collectivity in 54.4 GeV Au+Au collisions. Differences in v2 and v3 between baryons and anti-baryons are presented, and ratios of v3/v3/22 are studied and motivated by hydrodynamical calculations. The ratio of v2 of ϕ mesons to that of anti-protons (v2(ϕ)/v2(p¯)) shows centrality dependence at low transverse momentum, presumably resulting from the larger effects from hadronic interactions on anti-proton v2.
The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon γdir and neutral-pion (π0) triggers in p+p and central Au+Au collisions at sNN−−−√=200 GeV over a broad kinematic range, for jet resolution parameters R=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for R=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The magnitude of suppression is similar for γdir- and π0-triggered data, which constrains the color-charge and path-length dependence of jet quenching. Theoretical model calculations incorporating jet quenching do not fully describe the measurements.
Density fluctuations near the QCD critical point can be probed via an intermittency analysis in relativistic heavy-ion collisions. We report the first measurement of intermittency in Au+Au collisions at sNN−−−√ = 7.7-200 GeV measured by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The scaled factorial moments of identified charged hadrons are analyzed at mid-rapidity and within the transverse momentum phase space. We observe a power-law behavior of scaled factorial moments in Au+Au collisions and a decrease in the extracted scaling exponent (ν) from peripheral to central collisions. The ν is consistent with a constant for different collisions energies in the mid-central (10-40\%) collisions. Moreover, the ν in the 0-5\% most central Au+Au collisions exhibits a non-monotonic energy dependence that reaches a possible minimum around sNN−−−√ = 27 GeV. The physics implications on the QCD phase structure are discussed.
We report a measurement of exclusive J/ψ photoproduction in Au+Au ultra-peripheral collisions at sNN−−−√=200 GeV using the STAR detector. For the first time, i) the rapidity correlation between J/ψ photoproduction and neutron emission from nuclear breakups has been experimentally measured; ii) nuclear suppression factors are measured for both the coherent and incoherent J/ψ production. At photon-nucleon center-of-mass energy of 25.0 GeV, the coherent and incoherent J/ψ cross sections of Au nuclei are found to be 71±10% and 36±7%, respectively, of that of free protons. The stronger suppression observed in the incoherent production provides a new experimental handle to study the initial-state parton density in heavy nuclei. Data are compared with theoretical models quantitatively.
We report on the charged-particle multiplicity dependence of net-proton cumulant ratios up to sixth order from √s = 200 GeV p+p collisions at the Relativistic Heavy Ion Collider (RHIC). The measured ratios C4/C2, C5/C1, and C6/C2 decrease with increased charged-particle multiplicity and rapidity acceptance. Neither the Skellam baselines nor PYTHIA8 calculations account for the observed multiplicity dependence. In addition, the ratios C5/C1 and C6/C2 approach negative values in the highest-multiplicity events. The negative ratios in the most central p+p collisions at 200 GeV, similar to those observed in central Au+Au 200 GeV collisions, imply the formation of thermalized QCD matter.
With the STAR experiment at RHIC, we characterize √sNN = 200 GeV p+Au collisions by event activity (EA) measured within the pseudorapidity range η∈[−5,−3.4] in the Au-going direction and report correlations between this EA and hard- and soft-scale particle production at mid-rapidity (η∈[−1,1]). At the soft scale, charged particle production in low-EA p+Au collisions is comparable to that in \pp collisions and increases monotonically with increasing EA. At the hard scale, we report measurements of high transverse momentum (pT) jets in events of different EAs. In contrast to the soft particle production, high-pT particle production and EA are found to be inversely related. To investigate whether this is a signal of jet quenching in high-EA events, we also report ratios of pT imbalance and azimuthal separation of dijets in high- and low-EA events. Within our measurement precision, no significant differences are observed, disfavoring the presence of jet quenching in the highest 30% EA p+Au collisions at √sNN = 200 GeV.
A decisive experimental test of the Chiral Magnetic Effect (CME) is considered one of the major scientific goals at the Relativistic Heavy-Ion Collider (RHIC) towards understanding the nontrivial topological fluctuations of the Quantum Chromodynamics vacuum. In heavy-ion collisions, the CME is expected to result in a charge separation phenomenon across the reaction plane, whose strength could be strongly energy dependent. The previous CME searches have been focused on top RHIC energy collisions. In this Letter, we present a low energy search for the CME in Au+Au collisions at sNN−−−√=27 GeV. We measure elliptic flow scaled charge-dependent correlators relative to the event planes that are defined at both mid-rapidity |η|<1.0 and at forward rapidity 2.1<|η|<5.1. We compare the results based on the directed flow plane (Ψ1) at forward rapidity and the elliptic flow plane (Ψ2) at both central and forward rapidity. The CME scenario is expected to result in a larger correlation relative to Ψ1 than to Ψ2, while a flow driven background scenario would lead to a consistent result for both event planes[1,2]. In 10-50\% centrality, results using three different event planes are found to be consistent within experimental uncertainties, suggesting a flow driven background scenario dominating the measurement. We obtain an upper limit on the deviation from a flow driven background scenario at the 95\% confidence level. This work opens up a possible road map towards future CME search with the high statistics data from the RHIC Beam Energy Scan Phase-II.
In a Quark-Gluon Plasma (QGP), the fundamental building blocks of matter, quarks and gluons, are under extreme conditions of temperature and density. A QGP could exist in the early stages of the Universe, and in various objects and events in the cosmos. The thermodynamic and hydrodynamic properties of the QGP are described by Quantum Chromodynamics (QCD) and can be studied in heavy-ion collisions. Despite being a key thermodynamic parameter, the QGP temperature is still poorly known. Thermal lepton pairs (e+e− and μ+μ−) are ideal penetrating probes of the true temperature of the emitting source, since their invariant-mass spectra suffer neither from strong final-state interactions nor from blue-shift effects due to rapid expansion. Here we measure the QGP temperature using thermal e+e− production at the Relativistic Heavy Ion Collider (RHIC). The average temperature from the low-mass region (in-medium ρ0 vector-meson dominant) is (1.99±0.24)×1012 K, consistent with the chemical freeze-out temperature from statistical models and the phase transition temperature from LQCD. The average temperature from the intermediate mass region (above the ρ0 mass, QGP dominant) is significantly higher at (3.40±0.55)×1012 K. This work provides essential experimental thermodynamic measurements to map out the QCD phase diagram and understand the properties of matter under extreme conditions.