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- Acharya, Shreyasi (438)
- Adamová, Dagmar (438)
- Aglieri Rinella, Gianluca (438)
- Agnello, Michelangelo (438)
- Agrawal, Neelima (438)
- Ahammed, Zubayer (438)
- Ahmad, Shakeel (438)
- Akindinov, Alexander (438)
- Al-Turany, Mohammad (438)
- Aleksandrov, Dmitry (438)
- Alessandro, Bruno (438)
- Ali, Bushra (438)
- Alici, Andrea (438)
- Alkin, Anton (438)
- Alme, Johan (438)
- Alt, Torsten (438)
- Altsybeev, Igor (438)
- Andrei, Cristian (438)
- Andronic, Anton (438)
- Anguelov, Venelin (438)
- Antinori, Federico (438)
- Antonioli, Pietro (438)
- Apadula, Nicole (438)
- Arcelli, Silvia (438)
- Arnaldi, Roberta (438)
- Arsene, Ionut Cristian (438)
- Arslandok, Mesut (438)
- Augustinus, Andre (438)
- Badalà, Angela (438)
- Bailhache, Raphaëlle (438)
- Balbino, Alessandro (438)
- Baldisseri, Alberto (438)
- Banerjee, Debjani (438)
- Barioglio, Luca (438)
- Barth, Klaus (438)
- Bartsch, Esther (438)
- Bastid, Nicole (438)
- Basu, Sumit (438)
- Batigne, Guillaume (438)
- Batyunya, Boris (438)
- Bauri, Dibakar (438)
- Beattie, Caitlin (438)
- Belikov, Iouri (438)
- Bell Hechavarria, Ailec de la Caridad (438)
- Bellwied, Rene (438)
- Bencédi, Gyula (438)
- Beolè, Stefania (438)
- Betev, Latchezar (438)
- Bhasin, Anju (438)
- Bhattacharjee, Buddhadeb (438)
- Bianchi, Livio (438)
- Bielčík, Jaroslav (438)
- Bielčíková, Jana (438)
- Bilandzic, Ante (438)
- Biro, Gabor (438)
- Blau, Dmitry S. (438)
- Blume, Christoph (438)
- Boca, Gianluigi (438)
- Bock, Friederike (438)
- Bok, Jeongsu (438)
- Bombara, Marek (438)
- Bonomi, Germano (438)
- Borissov, Alexander (438)
- Botta, Elena (438)
- Bratrud, Lars (438)
- Braun-Munzinger, Peter (438)
- Bregant, Marco (438)
- Broz, Michal (438)
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- Bufalino, Stefania (438)
- Buthelezi, Edith Zinhle (438)
- Bühler, Paul (438)
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- Chinellato, David Dobrigkeit (438)
- Cho, Soyeon (438)
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- Christensen, Christian Holm (438)
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- Chujo, Tatsuya (438)
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- Clai, Giulia (438)
- Colella, Domenico (438)
- Colocci, Manuel (438)
- Conesa Balbastre, Gustavo (438)
- Contin, Giacomo (438)
- Cortese, Pietro (438)
- Costa, Filippo (438)
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- De Caro, Annalisa (438)
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- De Gruttola, Daniele (438)
- De Marco, Nora (438)
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- Dhankher, Preeti (438)
- Di Bari, Domenico (438)
- Di Mauro, Antonio (438)
- Dietel, Thomas (438)
- Ding, Yanchun (438)
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- Dmitrieva, Uliana (438)
- Dominguez Rosas, Edgar (438)
- Duarte Galvan, Carlos (438)
- Dubla, Andrea (438)
- Dupieux, Pascal (438)
- Elia, Domenico (438)
- Espagnon, Bruno (438)
- Eulisse, Giulio (438)
- Evans, David (438)
- Evdokimov, Sergey (438)
- Fabbietti, Laura (438)
- Faggin, Mattia (438)
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- Fasel, Markus (438)
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- Feofilov, Grigori A. (438)
- Fernández Téllez, Arturo (438)
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- Finogeev, Dmitry (438)
- Foertsch, Siegfried Valentin (438)
- Fokin, Sergey (438)
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- Furs, Artur (438)
- Gagliardi, Martino (438)
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- Germain, Marie (438)
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- Giubilato, Piero (438)
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- Graczykowski, Łukasz Kamil (438)
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- Große-Oetringhaus, Jan Fiete (438)
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- Haller, Barthélémy von (438)
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- Hassan, Hadi (438)
- Hatzifotiadou, Despina (438)
- Hauer, Philip (438)
- Hellbär, Ernst (438)
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- Hetland, Kristin Fanebust (438)
- Hillemanns, Hartmut (438)
- Hippolyte, Boris (438)
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- Humanic, Thomas J. (438)
- Ilkaev, Radiy (438)
- Inaba, Motoi (438)
- Ippolitov, Mikhail (438)
- Isakov, Artem (438)
- Ivanov, Marian (438)
- Jacazio, Nicolò (438)
- Jadlovska, Slavka (438)
- Jadlovsky, Jan (438)
- Jahnke, Cristiane (438)
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- Jonas, Florian (438)
- Jusko, Anton (438)
- Kalinak, Peter (438)
- Karavichev, Oleg V. (438)
- Karpechev, Evgeny (438)
- Kebschull, Udo (438)
- Keidel, Ralf (438)
- Keil, Markus (438)
- Ketzer, Bernhard (438)
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- Khanzadeev, Alexei (438)
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- Kisel, Ivan (438)
- Kiselev, Sergej N. (438)
- Klein, Jochen (438)
- Klein-Bösing, Christian (438)
- Kleiner, Matthias (438)
- Kluge, Alexander (438)
- Kobdaj, Chinorat (438)
- Kondratyev, Andrey (438)
- Kovalenko, Vladimir (438)
- Kowalski, Marek (438)
- Krivda, Marian (438)
- Krizek, Filip (438)
- Kryshen, Evgeny (438)
- Králik, Ivan (438)
- Kumar, Lokesh (438)
- Kundu, Sourav (438)
- Kurashvili, Podist (438)
- Kurepin, Alexander (438)
- Kushpil, Svetlana (438)
- Kwon, Youngil (438)
- König, Joshua Leon (438)
- La Rocca, Paola (438)
- Langoy, Rune (438)
- Larionov, Pavel (438)
- Laudi, Elisa (438)
- Lavicka, Roman (438)
- Lea, Ramona (438)
- Leeuwen, Marco van (438)
- Lehrbach, Johannes (438)
- Lietava, Roman (438)
- Lim, Bong-Hwi (438)
- Lindenstruth, Volker (438)
- Lippmann, Christian (438)
- Loizides, Constantinos (438)
- Lunardon, Marcello (438)
- Luparello, Grazia (438)
- López Torres, Ernesto (438)
- Ma, Yu-Gang (438)
- Mager, Magnus (438)
- Maire, Antonin (438)
- Malaev, Mikhail (438)
- Malinina, Liudmila (438)
- Mandaglio, Giuseppe (438)
- Manko, Vladislav (438)
- Manso, Franck (438)
- Mantovani Sarti, Valentina (438)
- Manzari, Vito (438)
- Mao, Yaxian (438)
- Margotti, Anselmo (438)
- Markert, Christina (438)
- Martinengo, Paolo (438)
- Masciocchi, Silvia (438)
- Masera, Massimo (438)
- Masoni, Alberto (438)
- Mastroserio, Annalisa (438)
- Matonoha, Oliver (438)
- Mazzaschi, Francesco (438)
- Mazzilli, Marianna (438)
- Melikyan, Yury (438)
- Meninno, Elisa (438)
- Meres, Michal (438)
- Miake, Yasuo (438)
- Micheletti, Luca (438)
- Mikhaylov, Konstantin (438)
- Modak, Abhi (438)
- Mohanty, Bedangadas (438)
- Mordasini, Cindy (438)
- Morozov, Igor (438)
- Morsch, Andreas (438)
- Mrnjavac, Teo (438)
- Muccifora, Valeria (438)
- Muhuri, Sanjib (438)
- Murakami, Hikari (438)
- Murray, Sean (438)
- Musa, Luciano (438)
- Musinsky, Jan (438)
- Nania, Rosario (438)
- Nappi, Eugenio (438)
- Nattrass, Christine (438)
- Neagu, Alexandra (438)
- Nellen, Lukas (438)
- Nikolaev, Sergey (438)
- Nikulin, Sergey (438)
- Nikulin, Vladimir (438)
- Noferini, Francesco (438)
- Nomokonov, Petr V. (438)
- Norman, Jaime (438)
- Novitzky, Norbert (438)
- Nowakowski, Piotr (438)
- Nyanin, Alexander (438)
- Nystrand, Joakim Ingemar (438)
- Ohlson, Alice (438)
- Oleniacz, Janusz (438)
- Oppedisano, Chiara (438)
- Ortiz Velasquez, Antonio (438)
- Oyama, Ken (438)
- Pachmayer, Yvonne C. (438)
- Pagano, Davide (438)
- Paul, Biswarup (438)
- Pei, Hua (438)
- Peitzmann, Thomas (438)
- Peng, Xinye (438)
- Pestov, Yury N. (438)
- Petrovici, Mihai A. (438)
- Piano, Stefano (438)
- Pikna, Miroslav (438)
- Pillot, Philippe (438)
- Pinazza, Ombretta (438)
- Pinsky, Lawrence (438)
- Pinto, Chiara (438)
- Pisano, Silvia (438)
- Planinic, Mirko (438)
- Pliquett, Fabian (438)
- Poghosyan, Martin G. (438)
- Poljak, Nikola (438)
- Pop, Amalia (438)
- Prino, Francesco (438)
- Pruneau, Claude A. (438)
- Pshenichnov, Igor A. (438)
- Puccio, Maximiliano (438)
- Quaglia, Luca (438)
- Ragoni, Simone (438)
- Ramello, Luciano (438)
- Rami, Fouad (438)
- Rath, Rutuparna (438)
- Ravasenga, Ivan (438)
- Redlich, Krzysztof (438)
- Reidt, Felix (438)
- Reygers, Klaus (438)
- Riegler, Werner (438)
- Ristea, Cătălin-Lucian (438)
- Rogochaya, Elena (438)
- Rojas Torres, Solangel (438)
- Ronchetti, Federico (438)
- Rossi, Andrea (438)
- Roy, Ankhi (438)
- Rui, Rinaldo (438)
- Rustamov, Anar (438)
- Ryabinkin, Evgeny (438)
- Röhrich, Dieter (438)
- Sadovskiy, Sergey (438)
- Sahoo, Raghunath (438)
- Sahoo, Sarita (438)
- Saini, Jogender (438)
- Sakai, Shingo (438)
- Sarma, Pranjal (438)
- Schicker, Rainer (438)
- Schmah, Alexander (438)
- Schmidt, Nicolas (438)
- Schukraft, Jürgen (438)
- Scioli, Gilda (438)
- Scomparin, Enrico (438)
- Sekiguchi, Yuko (438)
- Sekihata, Daiki (438)
- Selyuzhenkov, Ilya (438)
- Senyukov, Serhiy (438)
- Serebryakov, Dmitry (438)
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- Shabetai, Alexandre (438)
- Shahoyan, Ruben (438)
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- Shigaki, Kenta (438)
- Shirinkin, Sergey (438)
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- Siddhanta, Sabyasachi (438)
- Siemiarczuk, Teodor (438)
- Singhal, Vikas (438)
- Sitar, Branislav (438)
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- Taillepied, Guillaume (438)
- Takahashi, Jun (438)
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- Thomas, Deepa (438)
- Tikhonov, Anatoly (438)
- Toia, Alberica (438)
- Topilskaya, Nataliya (438)
- Toppi, Marco (438)
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- Tripathy, Tulika (438)
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- Usai, Gianluca (438)
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- Ahn, Sang Un (437)
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- Hadjidakis, Cynthia Marie (430)
- Harton, Austin Vincent (430)
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- Schmidt, Christian Joachim (430)
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- Schmidt, Marten Ole (430)
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- Bazo Alba, José Luis (429)
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- Mayer, Christoph (417)
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- Saha, Sumit Kumar (414)
- Mejia Camacho, Juan Manuel (412)
- Saarimäki, Oskari Antti Matti (412)
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- Sahoo, Baidyanath (408)
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- Jaelani, Syaefudin (406)
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- Doremalen, Lennart Vincent Rogier van (404)
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- Knospe, Anders Garritt (397)
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- Silva, Antonio Carlos Oliveira da (397)
- Klemenz, Thomas (393)
- Kuryakin, Alexey (392)
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- Tejeda Muñoz, Guillermo (392)
- Tumkin, Alexandr (392)
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- Zhou, You (390)
- Zhu, Jianhui (390)
- Gasik, Piotr (389)
- Godoy, Denise Aparecida Moreira de (389)
- Ivanov, Vladimir (389)
- Liu, Jian (389)
- Qiu, Shi (389)
- Tang, Siyu (389)
- Völkel, Benedikt (389)
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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 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) yield 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 2f0(980)/(π+ +π−) ratio. The prediction from the canonical statistical hadronisation 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.
The interaction between Λ baryons and kaons/antikaons is a crucial ingredient for the strangeness S=0 and S=−2 sector of the meson–baryon interaction at low energies. In particular, the ΛK‾ might help in understanding the origin of states such as the Ξ(1620), whose nature and properties are still under debate. Experimental data on Λ–K and Λ–K‾ systems are scarce, leading to large uncertainties and tension between the available theoretical predictions constrained by such data. In this Letter we present the measurements of Λ–K⊕+Λ‾–K− and Λ–K⊕−Λ‾–K+ correlations obtained in the high-multiplicity triggered data sample in pp collisions at s=13 TeV recorded by ALICE at the LHC. The correlation function for both pairs is modeled using the Lednický–Lyuboshits analytical formula and the corresponding scattering parameters are extracted. The Λ–K⊕−Λ‾–K+ correlations show the presence of several structures at relative momenta k⁎ above 200 MeV/c, compatible with the Ω baryon, the Ξ(1690), and Ξ(1820) resonances decaying into Λ–K− pairs. The low k⁎ region in the Λ–K⊕−Λ‾–K+ also exhibits the presence of the Ξ(1620) state, expected to strongly couple to the measured pair. The presented data allow to access the ΛK+ and ΛK− strong interaction with an unprecedented precision and deliver the first experimental observation of the Ξ(1620) decaying into ΛK−.
Multiplicity (Nch) distributions and transverse momentum (pT) spectra of inclusive primary charged particles in the kinematic range of |η|<0.8 and 0.15 GeV/c<pT<10 GeV/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. Providing these fundamental observables of bulk particle production consistently across a wide range of collision energies and system sizes can serve as an important input for tuning Monte Carlo event generators.
The most precise measurements to date of the 3ΛH lifetime τ and Λ separation energy BΛ are obtained using the data sample of Pb-Pb collisions at √sNN = 5.02 TeV collected by ALICE at the LHC. The 3ΛH is reconstructed via its charged two-body mesonic decay channel (3ΛH → 3He + π− and the charge-conjugate process). The measured values τ = [253 ± 11 (stat) ± 6 (syst)] ps and BΛ = [102 ± 63 (stat) ± 67 (syst)] keV are compatible with predictions from effective field theories and confirm that the 3ΛH structure is consistent with a weakly bound system.
The most precise measurements to date of the 3ΛH lifetime τ and Λ separation energy BΛ are obtained using the data sample of Pb-Pb collisions at √= 5.02 TeV collected by ALICE at the LHC. The 3ΛH is reconsNN structed via its charged two-body mesonic decay channel (3ΛH→ 3He + π− and the charge-conjugate process). The measured values τ=[253±11 (stat.)±6 (syst.)] ps and BΛ=[102±63 (stat.)±67 (syst.)] keV are compatible with predictions from effective field theories and confirm that the 3ΛH structure is consistent with a weakly-bound system.
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 ± 13 μb−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 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.
Results on the transverse spherocity dependence of light-flavor particle production (π, K, p, ϕ, K∗0, K0S, Λ, Ξ) at midrapidity in high-multiplicity pp collisions at s√=13 TeV were obtained with the ALICE apparatus. The transverse spherocity estimator (SpT=1O) categorizes events by their azimuthal topology. Utilizing narrow selections on SpT=1O, it is possible to contrast particle production in collisions dominated by many soft initial interactions with that observed in collisions dominated by one or more hard scatterings. Results are reported for two multiplicity estimators covering different pseudorapidity regions. The SpT=1O estimator is found to effectively constrain the hardness of the events when the midrapidity (|η|<0.8) estimator is used. The production rates of strange particles are found to be slightly higher for soft isotropic topologies, and severely suppressed in hard jet-like topologies. These effects are more pronounced for hadrons with larger mass and strangeness content, and observed when the topological selection is done within a narrow multiplicity interval. This demonstrates that an important aspect of the universal scaling of strangeness enhancement with final-state multiplicity is that high-multiplicity collisions are dominated by soft, isotropic processes. On the contrary, strangeness production in events with jet-like processes is significantly reduced. The results presented in this article are compared with several QCD-inspired Monte Carlo event generators. Models that incorporate a two-component phenomenology, either through mechanisms accounting for string density, or thermal production, are able to describe the observed strangeness enhancement as a function of SpT=1O.
Modification of charged-particle jets in event-shape engineered Pb–Pb collisions at √sNN = 5.02 TeV
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Charged-particle jet yields have been measured in semicentral Pb−Pb collisions at center-of-mass energy per nucleon-nucleon collision sNN−−−√=5 TeV with the ALICE detector at the LHC. These yields are reported as a function of the jet transverse momentum, and further classified by their angle with respect to the event plane and the event shape, characterized by ellipticity, in an effort to study the path-length dependence of jet quenching. Jets were reconstructed at midrapidity from charged-particle tracks using the anti-kT algorithm with resolution parameters R= 0.2 and 0.4, with event-plane angle and event-shape values determined using information from forward scintillating detectors. The results presented in this letter show that, in semicentral Pb−Pb collisions, there is no significant difference between jet yields in predominantly isotropic and elliptical events. However, out-of-plane jets are observed to be more suppressed than in-plane jets. Further, this relative suppression is greater for low transverse momentum (< 50 GeV/c) R= 0.2 jets produced in elliptical events, with out-of-plane to in-plane jet-yield ratios varying up to 5.2σ between different event-shape classes. These results agree with previous studies indicating that jets experience azimuthally anisotropic suppression when traversing the QGP medium, and can provide additional constraints on the path-length dependence of jet energy loss.
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.
Measurements of the production of electrons from heavy-flavour hadron decays in pp collisions at s√=13 TeV at midrapidity with the ALICE detector are presented down to a transverse momentum (pT) of 0.2 GeV/c and up to pT=35 GeV/c, which is the largest momentum range probed for inclusive electron measurements in ALICE. In p−Pb collisions, the production cross section and the nuclear modification factor of electrons from heavy-flavour hadron decays are measured in the pT range 0.5<pT<26 GeV/c at sNN−−−√=8.16 TeV. The nuclear modification factor is found to be consistent with unity within the statistical and systematic uncertainties. In both collision systems, first measurements of the yields of electrons from heavy-flavour hadron decays in different multiplicity intervals normalised to the multiplicity-integrated yield (self-normalised yield) at midrapidity are reported as a function of the self-normalised charged-particle multiplicity estimated at midrapidity. The self-normalised yields in pp and p−Pb collisions grow faster than linear with the self-normalised multiplicity. A strong pT dependence is observed in pp collisions, where the yield of high-pT electrons increases faster as a function of multiplicity than the one of low-pT electrons. The measurement in p−Pb collisions shows no pT dependence within uncertainties. The self-normalised yields in pp and p−Pb collisions are compared with measurements of other heavy-flavour, light-flavour, and strange particles, and with Monte Carlo simulations.
This Letter presents the first measurement of event-by-event fluctuations of the net number (difference between the particle and antiparticle multiplicities) of multistrange hadrons Ξ− and Ξ¯¯¯¯+ and its correlation with the net-kaon number using the data collected by the ALICE Collaboration in pp, p−Pb, and Pb−Pb collisions at a center-of-mass energy per nucleon pair sNN−−−√=5.02 TeV. The statistical hadronization model with a correlation over three units of rapidity between hadrons having the same and opposite strangeness content successfully describes the results. On the other hand, string-fragmentation models that mainly correlate strange hadrons with opposite strange quark content over a small rapidity range fail to describe the data.
he first measurement of 3ΛH and 3Λ¯¯¯¯H¯¯¯¯ differential production with respect to transverse momentum and centrality in Pb−Pb collisions at sNN−−−√=5.02~TeV is presented. The 3ΛH has been reconstructed via its two-charged-body decay channel, i.e., 3ΛH→3He+π−. A Blast-Wave model fit of the pT-differential spectra of all nuclear species measured by the ALICE collaboration suggests that the 3ΛH kinetic freeze-out surface is consistent with that of other nuclei. The ratio between the integrated yields of 3ΛH and 3He is compared to predictions from the statistical hadronisation model and the coalescence model, with the latter being favoured by the presented measurements.
First measurements of hadron(h)−Λ azimuthal angular correlations in p−Pb collisions at sNN−−−√ = 5.02 TeV using the ALICE detector at the LHC are presented. These correlations are used to separate the production of associated Λ baryons into three different kinematic regions, namely those produced in the direction of the trigger particle (near-side), those produced in the opposite direction (away-side), and those whose production is uncorrelated with the jet-axis (underlying event). The per-trigger associated Λ yields in these regions are extracted, along with the near- and away-side azimuthal peak widths, and the results are studied as a function of associated particle pT and event multiplicity. Comparisons with the DPMJET event generator and previous measurements of the ϕ(1020) meson are also made. The final results indicate that strangeness production in the highest multiplicity p−Pb collisions is enhanced relative to low multiplicity collisions in the jet-like regions, as well as the underlying event. The production of Λ relative to charged hadrons is also enhanced in the underlying event when compared to the jet-like regions. Additionally, the results hint that strange quark production in the away-side of the jet is modified by soft interactions with the underlying event.
Measurements of (anti)deuteron and (anti)3He production in the rapidity range |y|< 0.5 as a function of the transverse momentum and event multiplicity in Xe−Xe collisions at a center-of-mass energy per nucleon−nucleon pair of sNN−−−√ = 5.44 TeV are presented. The coalescence parameters B2 and B3 are measured as a function of the transverse momentum per nucleon. The ratios between (anti)deuteron and (anti)3He yields and those of (anti)protons and pions are reported as a function of the mean charged-particle multiplicity density, and compared with two implementations of the statistical hadronization model (SHM) and with coalescence predictions. The elliptic flow of (anti)deuterons is measured for the first time in Xe−Xe collisions and shows features similar to those already observed in Pb−Pb collisions, i.e., the mass ordering at low transverse momentum and the meson−baryon grouping at intermediate transverse momentum. The production of nuclei is particularly sensitive to the chemical freeze-out temperature of the system created in the collision, which is extracted from a grand-canonical-ensemble-based thermal fit, performed for the first time including light nuclei along with light-flavor hadrons in Xe−Xe collisions. The extracted chemical freeze-out temperature Tchem = (154.2 ± 1.1) MeV in Xe−Xe collisions is similar to that observed in Pb−Pb collisions and close to the crossover temperature predicted by lattice QCD calculations.
The transverse momentum (pT) differential production cross section of the promptly-produced charm-strange baryon Ξ0c (and its charge conjugate Ξ0c¯¯¯¯¯¯) is measured at midrapidity via its hadronic decay into π+Ξ− in p−Pb collisions at a centre-of-mass energy per nucleon−nucleon collision sNN−−−√ = 5.02 TeV with the ALICE detector at the LHC. The Ξ0c nuclear modification factor (RpPb), calculated from the cross sections in pp and p−Pb collisions, is presented and compared with the RpPb of Λ+c baryons. The ratios between the pT-differential production cross section of Ξ0c baryons and those of D0 mesons and Λ+c baryons are also reported and compared with results at forward and backward rapidity from the LHCb Collaboration. The measurements of the production cross section of prompt Ξ0c baryons are compared with a model based on perturbative QCD calculations of charm-quark production cross sections, which includes only cold nuclear matter effects in p−Pb collisions, and underestimates the measurement by a factor of about 50. This discrepancy is reduced when the data is compared with a model in which hadronisation is implemented via quark coalescence. The pT-integrated cross section of prompt Ξ0c-baryon production at midrapidity extrapolated down to pT = 0 is also reported. These measurements offer insights and constraints for theoretical calculations of the hadronisation process. Additionally, they provide inputs for the calculation of the charm production cross section in p−Pb collisions at midrapidity.
Investigating strangeness enhancement with multiplicity in pp collisions using angular correlations
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A study of strange hadron production associated with hard scattering processes and with the underlying event is conducted to investigate the origin of the enhanced production of strange hadrons in small collision systems characterised by large charged-particle multiplicities. For this purpose, the production of the single-strange meson K0S and the double-strange baryon Ξ± is measured, in each event, in the azimuthal direction of the highest-pT particle (``trigger" particle), related to hard scattering processes, and in the direction transverse to it in azimuth, associated with the underlying event, in pp collisions at s√=5.02 TeV and s√=13 TeV using the ALICE detector at the LHC. The per-trigger yields of K0S and Ξ± are dominated by the transverse-to-leading production (i.e., in the direction transverse to the trigger particle), whose contribution relative to the toward-leading production is observed to increase with the event charged-particle multiplicity. The transverse-to-leading and the toward-leading Ξ±/K0S yield ratios increase with the multiplicity of charged particles, suggesting that strangeness enhancement with multiplicity is associated with both hard scattering processes and the underlying event. The relative production of Ξ± with respect to K0S is higher in transverse-to-leading processes over the whole multiplicity interval covered by the measurement. The K0S and Ξ± per-trigger yields and yield ratios are compared with predictions of three different phenomenological models, namely PYTHIA 8.2 with the Monash tune, PYTHIA 8.2 with ropes and EPOS LHC. The comparison shows that none of them can quantitatively describe either the transverse-to-leading or the toward-leading yields of K0S and Ξ±.
The first measurement of the impact-parameter dependent angular anisotropy in the decay of coherently photoproduced ρ0 mesons is presented. The ρ0 mesons are reconstructed through their decay into a pion pair. The measured anisotropy corresponds to the amplitude of the cos(2ϕ) modulation, where ϕ is the angle between the two vectors formed by the sum and the difference of the transverse momenta of the pions, respectively. The measurement was performed by the ALICE Collaboration at the LHC using data from ultraperipheral Pb−Pb collisions at a center-of-mass energy of sNN−−−√ = 5.02 TeV per nucleon pair. Different impact-parameter regions are selected by classifying the events in nuclear-breakup classes. The amplitude of the cos(2ϕ) modulation is found to increase by about one order of magnitude from large to small impact parameters. Theoretical calculations, which describe the measurement, explain the cos(2ϕ) anisotropy as the result of a quantum interference effect at the femtometer scale that arises from the ambiguity as to which of the nuclei is the source of the photon in the interaction.