Ontology type: schema:ScholarlyArticle Open Access: True
2019-04-04
AUTHORSS. Acharya, F.-T. Acosta, D. Adamová, S. P. Adhya, A. Adler, J. Adolfsson, M. M. Aggarwal, G. Aglieri Rinella, M. Agnello, Z. Ahammed, S. Ahmad, S. U. Ahn, S. Aiola, A. Akindinov, M. Al-Turany, S. N. Alam, D. S. D. Albuquerque, D. Aleksandrov, B. Alessandro, H. M. Alfanda, R. Alfaro Molina, Y. Ali, A. Alici, A. Alkin, J. Alme, T. Alt, L. Altenkamper, I. Altsybeev, M. N. Anaam, C. Andrei, D. Andreou, H. A. Andrews, A. Andronic, M. Angeletti, V. Anguelov, C. Anson, T. Antičić, F. Antinori, P. Antonioli, R. Anwar, N. Apadula, L. Aphecetche, H. Appelshäuser, S. Arcelli, R. Arnaldi, M. Arratia, I. C. Arsene, M. Arslandok, A. Augustinus, R. Averbeck, M. D. Azmi, A. Badalà, Y. W. Baek, S. Bagnasco, R. Bailhache, R. Bala, A. Baldisseri, M. Ball, R. C. Baral, R. Barbera, L. Barioglio, G. G. Barnaföldi, L. S. Barnby, V. Barret, P. Bartalini, K. Barth, E. Bartsch, N. Bastid, S. Basu, G. Batigne, B. Batyunya, P. C. Batzing, D. Bauri, J. L. Bazo Alba, I. G. Bearden, H. Beck, C. Bedda, N. K. Behera, I. Belikov, F. Bellini, H. Bello Martinez, R. Bellwied, L. G. E. Beltran, V. Belyaev, G. Bencedi, S. Beole, A. Bercuci, Y. Berdnikov, D. Berenyi, R. A. Bertens, D. Berzano, L. Betev, A. Bhasin, I. R. Bhat, H. Bhatt, B. Bhattacharjee, A. Bianchi, L. Bianchi, N. Bianchi, J. Bielčík, J. Bielčíková, A. Bilandzic, G. Biro, R. Biswas, S. Biswas, J. T. Blair, D. Blau, C. Blume, G. Boca, F. Bock, A. Bogdanov, L. Boldizsár, A. Bolozdynya, M. Bombara, G. Bonomi, M. Bonora, H. Borel, A. Borissov, M. Borri, E. Botta, C. Bourjau, L. Bratrud, P. Braun-Munzinger, M. Bregant, T. A. Broker, M. Broz, E. J. Brucken, E. Bruna, G. E. Bruno, D. Budnikov, H. Buesching, S. Bufalino, P. Buhler, P. Buncic, O. Busch, Z. Buthelezi, J. B. Butt, J. T. Buxton, J. Cabala, D. Caffarri, H. Caines, A. Caliva, E. Calvo Villar, R. S. Camacho, P. Camerini, A. A. Capon, F. Carnesecchi, J. Castillo Castellanos, A. J. Castro, E. A. R. Casula, C. Ceballos Sanchez, P. Chakraborty, S. Chandra, B. Chang, W. Chang, S. Chapeland, M. Chartier, S. Chattopadhyay, S. Chattopadhyay, A. Chauvin, C. Cheshkov, B. Cheynis, V. Chibante Barroso, D. D. Chinellato, S. Cho, P. Chochula, T. Chowdhury, P. Christakoglou, C. H. Christensen, P. Christiansen, T. Chujo, C. Cicalo, L. Cifarelli, F. Cindolo, J. Cleymans, F. Colamaria, D. Colella, A. Collu, M. Colocci, M. Concas, G. Conesa Balbastre, Z. Conesa del Valle, J. G. Contreras, T. M. Cormier, Y. Corrales Morales, P. Cortese, M. R. Cosentino, F. Costa, S. Costanza, J. Crkovská, P. Crochet, E. Cuautle, L. Cunqueiro, D. Dabrowski, T. Dahms, A. Dainese, F. P. A. Damas, S. Dani, M. C. Danisch, A. Danu, D. Das, I. Das, S. Das, A. Dash, S. Dash, S. De, A. De Caro, G. de Cataldo, C. de Conti, J. de Cuveland, A. De Falco, D. De Gruttola, N. De Marco, S. De Pasquale, R. D. De Souza, H. F. Degenhardt, A. Deisting, A. Deloff, S. Delsanto, P. Dhankher, D. Di Bari, A. Di Mauro, R. A. Diaz, T. Dietel, P. Dillenseger, Y. Ding, R. Divià, Ø. Djuvsland, A. Dobrin, D. Domenicis Gimenez, B. Dönigus, O. Dordic, A. K. Dubey, A. Dubla, S. Dudi, A. K. Duggal, M. Dukhishyam, P. Dupieux, R. J. Ehlers, D. Elia, H. Engel, E. Epple, B. Erazmus, F. Erhardt, A. Erokhin, M. R. Ersdal, B. Espagnon, G. Eulisse, J. Eum, D. Evans, S. Evdokimov, L. Fabbietti, M. Faggin, J. Faivre, A. Fantoni, M. Fasel, L. Feldkamp, A. Feliciello, G. Feofilov, A. Fernández Téllez, A. Ferrero, A. Ferretti, A. Festanti, V. J. G. Feuillard, J. Figiel, S. Filchagin, D. Finogeev, F. M. Fionda, G. Fiorenza, F. Flor, M. Floris, S. Foertsch, P. Foka, S. Fokin, E. Fragiacomo, A. Francisco, U. Frankenfeld, G. G. Fronze, U. Fuchs, C. Furget, A. Furs, M. Fusco Girard, J. J. Gaardhøje, M. Gagliardi, A. M. Gago, K. Gajdosova, C. D. Galvan, P. Ganoti, C. Garabatos, E. Garcia-Solis, K. Garg, C. Gargiulo, K. Garner, P. Gasik, E. F. Gauger, M. B. Gay Ducati, M. Germain, J. Ghosh, P. Ghosh, S. K. Ghosh, P. Gianotti, P. Giubellino, P. Giubilato, P. Glässel, D. M. Goméz Coral, A. Gomez Ramirez, V. 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Ivanov, V. Izucheev, B. Jacak, N. Jacazio, P. M. Jacobs, M. B. Jadhav, S. Jadlovska, J. Jadlovsky, S. Jaelani, C. Jahnke, M. J. Jakubowska, M. A. Janik, M. Jercic, O. Jevons, R. T. Jimenez Bustamante, M. Jin, P. G. Jones, A. Jusko, P. Kalinak, A. Kalweit, J. H. Kang, V. Kaplin, S. Kar, A. Karasu Uysal, O. Karavichev, T. Karavicheva, P. Karczmarczyk, E. Karpechev, U. Kebschull, R. Keidel, M. Keil, B. Ketzer, Z. Khabanova, A. M. Khan, S. Khan, S. A. Khan, A. Khanzadeev, Y. Kharlov, A. Khatun, A. Khuntia, M. M. Kielbowicz, B. Kileng, B. Kim, B. Kim, D. Kim, D. J. Kim, E. J. Kim, H. Kim, J. S. Kim, J. Kim, J. Kim, M. Kim, S. Kim, T. Kim, T. Kim, K. Kindra, S. Kirsch, I. Kisel, S. Kiselev, A. Kisiel, J. L. Klay, C. Klein, J. Klein, S. Klein, C. Klein-Bösing, S. Klewin, A. Kluge, M. L. Knichel, A. G. Knospe, C. Kobdaj, M. Kofarago, M. K. Köhler, T. Kollegger, N. Kondratyeva, E. Kondratyuk, P. J. Konopka, M. Konyushikhin, L. Koska, O. Kovalenko, V. Kovalenko, M. Kowalski, I. Králik, A. Kravčáková, L. Kreis, M. Krivda, F. Krizek, M. Krüger, E. Kryshen, M. Krzewicki, A. M. Kubera, V. Kučera, C. Kuhn, P. G. Kuijer, J. Kumar, L. Kumar, S. Kumar, S. Kundu, P. Kurashvili, A. Kurepin, A. B. Kurepin, S. Kushpil, J. Kvapil, M. J. Kweon, Y. Kwon, S. L. La Pointe, P. La Rocca, Y. S. Lai, R. Langoy, K. Lapidus, A. Lardeux, P. Larionov, E. Laudi, R. Lavicka, T. Lazareva, R. Lea, L. Leardini, S. Lee, F. Lehas, S. Lehner, J. Lehrbach, R. C. Lemmon, I. León Monzón, P. Lévai, X. Li, X. L. Li, J. Lien, R. Lietava, B. Lim, S. Lindal, V. Lindenstruth, S. W. Lindsay, C. Lippmann, M. A. Lisa, V. Litichevskyi, A. Liu, H. M. Ljunggren, W. J. Llope, D. F. Lodato, V. Loginov, C. Loizides, P. Loncar, X. Lopez, E. López Torres, P. Luettig, J. R. Luhder, M. Lunardon, G. Luparello, M. Lupi, A. Maevskaya, M. Mager, S. M. Mahmood, A. Maire, R. D. Majka, M. Malaev, Q. W. Malik, L. Malinina, D. Mal’Kevich, P. Malzacher, A. Mamonov, V. Manko, F. Manso, V. Manzari, Y. Mao, M. Marchisone, J. Mareš, G. 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Zhu, A. Zichichi, M. B. Zimmermann, G. Zinovjev, N. Zurlo
ABSTRACTThe pseudorapidity density of charged particles, dNch/dη\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {d}N_{\mathrm{ch}}/\mathrm {d}\eta $$\end{document}, in p–Pb collisions has been measured at a centre-of-mass energy per nucleon–nucleon pair of sNN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s_{\scriptscriptstyle {\mathrm{NN}}}}$$\end{document} = 8.16 TeV at mid-pseudorapidity for non-single-diffractive events. The results cover 3.6 units of pseudorapidity, |η|<1.8\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$|\eta |<1.8$$\end{document}. The dNch/dη\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {d}N_{\mathrm{ch}}/\mathrm {d}\eta $$\end{document} value is 19.1±0.7\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$19.1\pm 0.7$$\end{document} at |η|<0.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$|\eta |<0.5$$\end{document}. This quantity divided by ⟨Npart⟩\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle N_{\mathrm{part}} \rangle $$\end{document} / 2 is 4.73±0.20\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$4.73\pm 0.20$$\end{document}, where ⟨Npart⟩\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\langle N_{\mathrm{part}} \rangle $$\end{document}is the average number of participating nucleons, is 9.5% higher than the corresponding value for p–Pb collisions at sNN\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sqrt{s_{\scriptscriptstyle {\mathrm{NN}}}}$$\end{document} = 5.02 TeV. Measurements are compared with models based on different mechanisms for particle production. All models agree within uncertainties with data in the Pb-going side, while HIJING overestimates, showing a symmetric behaviour, and EPOS underestimates the p-going side of the dNch/dη\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {d}N_{\mathrm{ch}}/\mathrm {d}\eta $$\end{document} distribution. Saturation-based models reproduce the distributions well for η>-1.3\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\eta >-1.3$$\end{document}. The dNch/dη\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {d}N_{\mathrm{ch}}/\mathrm {d}\eta $$\end{document} is also measured for different centrality estimators, based both on the charged-particle multiplicity and on the energy deposited in the Zero-Degree Calorimeters. A study of the implications of the large multiplicity fluctuations due to the small number of participants for systems like p–Pb in the centrality calculation for multiplicity-based estimators is discussed, demonstrating the advantages of determining the centrality with energy deposited near beam rapidity. More... »
PAGES307
http://scigraph.springernature.com/pub.10.1140/epjc/s10052-019-6801-9
DOIhttp://dx.doi.org/10.1140/epjc/s10052-019-6801-9
DIMENSIONShttps://app.dimensions.ai/details/publication/pub.1113269068
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