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K*(892)0 and Φ(1020) Production In

S. Das,Dagmar Adamová, Alexander Adler,Jonatan Adolfsson,Gianluca Aglieri Rinella,Michelangelo Agnello,Neelima Agrawal, Z. Ahammed, S. Ahmad,Sang Un Ahn,Ishaan Ahuja,Zaenal Akbar, Alexander Akindinov, Mohammad Al-Turany, Sk Noor Alam, D. Aleksandrov,Bruno Alessandro,Haidar Mas'Ud Alfanda, R. Alfaro Molina,Bushra Ali, Yasir Ali,Andrea Alici,Negin Alizadehvandchali,Anton Alkin,Johan Alme, Torsten Alt, Igor Altsybeev,Mustafa Anaam,Cristian Andrei,Dimitra Andreou,Anton Andronic,Massimo Angeletti, Venelin Anguelov,Federico Antinori, P. Antonioli,C Anuj, Nicole Apadula,Laurent Bernard Aphecetche, H. Appelshäuser, S. Arcelli,Roberta Arnaldi, Ionut Cristian Arsene,Mesut Arslandok, A. Augustinus, R. 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Physical review C(2023)

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Abstract
The production of $\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ resonances has been measured in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV using the ALICE detector. Resonances are reconstructed via their hadronic decay channels in the rapidity interval $-$0.5 $<$ $y$ $<$ 0 and the transverse momentum spectra are measured for various multiplicity classes up to $p_{\rm T}$ = 20 GeV/$c$ for $\mathrm{K}^{*}(\mathrm{892})^{0}$ and $p_{\rm T}$ = 16 GeV/$c$ for $\mathrm{\phi(1020)}$. The $p_{\rm T}$ -integrated yields and mean transverse momenta are reported and compared with previous results in pp, p-Pb and Pb-Pb collisions. The $x_{\mathrm{T}}$ scaling for $\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ resonance production is newly tested in p-Pb collisions and found to hold in the high-$p_{\rm T}$ region at Large Hadron Collider energies. The nuclear modification factors ($R_{\rm pPb}$) as a function of $p_{\rm T}$ for $\mathrm{K}^{*0}$ and $\mathrm{\phi}$ at $\sqrt{s_{NN}}$ = 8.16 TeV are presented along with the new $R_{\rm pPb}$ measurements of $\mathrm{K}^{*0}$, $\mathrm{\phi}$ , $\Xi$, and $\Omega$ at $\sqrt{s_{\rm NN}}$ = 5.02 TeV. At intermediate $p_{\rm T}$ (2-8 GeV/$c$), $R_{\rm pPb}$ of $\Xi$, $\Omega$ show a Cronin-like enhancement, while $\mathrm{K}^{*0}$ and $\mathrm{\phi}$ show no or little nuclear modification. At high $p_{\rm T}$ ($>$ 8 GeV/$c$), the $R_{\rm pPb}$ values of all hadrons are consistent with unity within uncertainties. The $R_{\rm pPb}$ of $\mathrm{K}^{*}(\mathrm{892})^{0}$ and $\mathrm{\phi(1020)}$ at $\sqrt{s_{\rm NN}}$ = 8.16 and 5.02 TeV show no significant energy dependence.
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