Production of K * ( 892 ) 0 and ϕ ( 1020 ) in p p   and   Pb − Pb collisions at s N N = 5.02   TeV

Acharya, S.; Adamová, D.; Adler, A.; Adolfsson, J.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahmad, S.; Ahn, S. U.; Ahuja, I.; Akbar, Z.; Akindinov, A.; Al-Turany, M.; Alam, S. N.; Aleksandrov, D.; Alessandro, B.; Alfanda, H. M.; Alfaro Molina, R.; Ali, B.; Ali, Y.; Alici, A.; Alizadehvandchali, N.; Alkin, A.; Alme, J.; Alt, T.; Altenkamper, L.; Altsybeev, I.; Anaam, M. N.; Andrei, C.; Andreou, D.; Andronic, A.; Angeletti, M.; Anguelov, V.; Antinori, F.; Antonioli, P.; Anuj, C.; Apadula, N.; Aphecetche, L.; Appelshäuser, H.; Arcelli, S.; Arnaldi, R.; Arsene, I. C.; Arslandok, M.; Augustinus, A.; Averbeck, R.; Aziz, S.; Azmi, M. D.; Badalà, A.; Baek, Y. W.; Bai, X.; Bailhache, R.; Bailung, Y.; Bala, R.; Balbino, A.; Baldisseri, A.; Balis, B.; Ball, M.; Banerjee, D.; Barbera, R.; Barioglio, L.; Barlou, M.; Barnaföldi, G. G.; Barnby, L. 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B.; Bysiak, S. A.; Caffarri, D.; Cai, M.; Caines, H.; Caliva, A.; Calvo Villar, E.; Camacho, J. M. M.; Camacho, R. S.; Camerini, P.; Canedo, F. D. M.; Carnesecchi, F.; Caron, R.; Castillo Castellanos, J.; Casula, E. A. R.; Catalano, F.; Ceballos Sanchez, C.; Chakraborty, P.; Chandra, S.; Chapeland, S.; Chartier, M.; Chattopadhyay, S.; Chattopadhyay, S.; Chauvin, A.; Chavez, T. G.; Cheshkov, C.; Cheynis, B.; Chibante Barroso, V.; Chinellato, D. D.; Cho, S.; Chochula, P.; Christakoglou, P.; Christensen, C. H.; Christiansen, P.; Chujo, T.; Cicalo, C.; Cifarelli, L.; Cindolo, F.; Ciupek, M. R.; Clai, G.; Cleymans, J.; Colamaria, F.; Colburn, J. S.; Colella, D.; Collu, A.; Colocci, M.; Concas, M.; Conesa Balbastre, G.; Conesa del Valle, Z.; Contin, G.; Contreras, J. G.; Coquet, M. L.; Cormier, T. M.; Cortese, P.; Cosentino, M. R.; Costa, F.; Costanza, S.; Crochet, P.; Cuautle, E.; Cui, P.; Cunqueiro, L.; Dainese, A.; Damas, F. P. A.; Danisch, M. C.; Danu, A.; Das, I.; Das, P.; Das, P.; Das, S.; Dash, A.; Dash, S.; De, S.; De Caro, A.; de Cataldo, G.; De Cilladi, L.; de Cuveland, J.; De Falco, A.; De Gruttola, D.; De Marco, N.; De Martin, C.; De Pasquale, S.; Deb, S.; Degenhardt, H. F.; Deja, K. R.; Dello Stritto, L.; Delsanto, S.; Deng, W.; Dhankher, P.; Di Bari, D.; Di Mauro, A.; Diaz, R. A.; Dietel, T.; Ding, Y.; Divià, R.; Dixit, D. U.; Djuvsland, Ø.; Dmitrieva, U.; Do, J.; Dobrin, A.; Dönigus, B.; Dordic, O.; Dubey, A. K.; Dubla, A.; Dudi, S.; Dukhishyam, M.; Dupieux, P.; Dzalaiova, N.; Eder, T. M.; Ehlers, R. J.; Eikeland, V. N.; Elia, D.; Erazmus, B.; Ercolessi, F.; Erhardt, F.; Erokhin, A.; Ersdal, M. R.; Espagnon, B.; Eulisse, G.; Evans, D.; Evdokimov, S.; Fabbietti, L.; Faggin, M.; Faivre, J.; Fan, F.; Fantoni, A.; Fasel, M.; Fecchio, P.; Feliciello, A.; Feofilov, G.; Fernández Téllez, A.; Ferrero, A.; Ferretti, A.; Feuillard, V. J. G.; Figiel, J.; Filchagin, S.; Finogeev, D.; Fionda, F. 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doi:10.1103/PhysRevC.106.034907

Title: Production of $K^{*} {(892)}^{0}$ and $ϕ (1020)$ in $p p and Pb − Pb$ collisions at $\sqrt{s_{N N}} = 5.02 TeV$

Journal Article · Wed Sep 14 00:00:00 EDT 2022 · Physical Review C

DOI:https://doi.org/10.1103/PhysRevC.106.034907· OSTI ID:1887317

Acharya, S.; Adamová, D.; Adler, A.; Adolfsson, J.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahmad, S.; Ahn, S. U.; Ahuja, I.; Akbar, Z.; Akindinov, A.; Al-Turany, M.; Alam, S. N.; Aleksandrov, D.; Alessandro, B.; Alfanda, H. M.; Alfaro Molina, R.; Ali, B. more »

The production of K*(892)⁰ and φ(1020) mesons in proton–proton (pp) and lead–lead (Pb–Pb) collisions at $$\sqrt{s{NN}}$$ = 5.02 TeV has been measured using the ALICE detector at the Large Hadron Collider (LHC). The transverse momentum (p_T) distributions of K*(892)⁰ and φ(1020) mesons have been measured at midrapidity (|y|<0.5) up to p_T= 20 GeV/c in inelastic pp collisions and for several Pb–Pb collision centralities. The collision centrality and collision energy dependence of the average transverse momenta agree with the radial flow scenario observed with stable hadrons, showing that the effect is stronger for more central collisions and higher collision energies. The K*⁰/K ratio is found to be suppressed in Pb–Pb collisions relative to pp collisions: this indicates a loss of the measured K*(892)⁰ signal due to rescattering of its decay products in the hadronic phase. In contrast, for the longer-lived φ(1020) mesons, no such suppression is observed. The nuclear modification factors (R_AA) of K*(892)⁰ and φ(1020) mesons are calculated using pp reference spectra at the same collision energy. In central Pb–Pb collisions for p_T > 8 GeV/c, the R_AA values of K*(892)⁰ and φ(1020) are below unity and observed to be similar to those of pions, kaons, and (anti)protons. The R_AA values at high p_T (>8 GeV/c) for K*(892)⁰ and φ(1020) mesons are in agreement within uncertainties for $$\sqrt{s{NN}}$$= 5.02 and 2.76 TeV.

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Research Organization:: Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); Univ. of Tennessee, Knoxville, TN (United States)

Sponsoring Organization:: USDOE Office of Science (SC), Nuclear Physics (NP)

Contributing Organization:: ALICE Collaboration

Grant/Contract Number:: AC05-00OR22725; AC02-05CH11231; FG02-96ER40982

OSTI ID:: 1887317

Alternate ID(s):: OSTI ID: 1896969; OSTI ID: 1924465; OSTI ID: 2007929

Journal Information:: Physical Review C, Journal Name: Physical Review C Vol. 106 Journal Issue: 3; ISSN 2469-9985

Publisher:: American Physical SocietyCopyright Statement

Country of Publication:: United States

Language:: English

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Production of light-flavor hadrons in pp collisions at $$\sqrt{s}~=~7\text { and }\sqrt{s} = 13 \, \text { TeV} $$ Acharya, S.; Adamová, D.; Adler, A. The European Physical Journal C, Vol. 81, Issue 3 https://doi.org/10.1140/epjc/s10052-020-08690-5	journal	March 2021

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73 NUCLEAR PHYSICS AND RADIATION PHYSICS
hadron-hadron interactions
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Title: Production of K * ( 892 ) 0 and ϕ ( 1020 ) in p p and Pb − Pb collisions at s N N = 5.02 TeV

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Title: Production of $K^{*} {(892)}^{0}$ and $ϕ (1020)$ in $p p and Pb − Pb$ collisions at $\sqrt{s_{N N}} = 5.02 TeV$