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The production of K∗ (892) 0 and φ(1020) mesons in proton–proton (pp) and lead–lead (Pb–Pb) collisions at √s NN = 5.02 TeV has been measured using the ALICE detector at the Large Hadron Collider (LHC). The transverse momentum (pT ) distributions of K∗ (892) 0 and φ(1020) mesons have been measured at midrapidity (|y| < 0.5) up to pT = 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 pT > 8 GeV/c, the RAA 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 RAA values at high pT (>8 GeV/c) for K∗ (892) 0 and φ(1020) mesons are in agreement within uncertainties for √s NN = 5.02 and 2.76 TeV.
S. Acharya, D. Adamov??, A. Adler, J. Adolfsson, G. Aglieri Rinella, M. Agnello, et al. (2022). Production of K*(892)0 and φ(1020) in pp and Pb-Pb collisions at √sNN=5.02 TeV. PHYSICAL REVIEW C, 106(3), 1-20 [10.1103/physrevc.106.034907].
Production of K*(892)0 and φ(1020) in pp and Pb-Pb collisions at √sNN=5.02 TeV
S. Acharya;D. Adamov??;A. Adler;J. Adolfsson;G. Aglieri Rinella;M. Agnello;N. Agrawal;Z. Ahammed;S. Ahmad;S. U. Ahn;I. Ahuja;Z. Akbar;A. Akindinov;M. Al-Turany;S. N. Alam;D. Aleksandrov;B. Alessandro;H. M. Alfanda;R. Alfaro Molina;B. Ali;Y. Ali;A. Alici;N. Alizadehvandchali;A. Alkin;J. Alme;T. Alt;L. Altenkamper;I. Altsybeev;M. N. Anaam;C. Andrei;D. Andreou;A. Andronic;M. Angeletti;V. Anguelov;F. Antinori;P. Antonioli;C. Anuj;N. Apadula;L. Aphecetche;H. Appelsh??user;S. Arcelli;R. Arnaldi;I. C. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;S. Aziz;M. D. Azmi;A. Badal??;Y. W. Baek;X. Bai;R. Bailhache;Y. Bailung;R. Bala;A. Balbino;A. Baldisseri;B. Balis;M. Ball;D. Banerjee;R. Barbera;L. Barioglio;M. Barlou;G. G. Barnaf??ldi;L. S. Barnby;V. Barret;C. Bartels;K. Barth;E. Bartsch;F. Baruffaldi;N. Bastid;S. Basu;G. Batigne;B. Batyunya;D. Bauri;J. L. Bazo Alba;I. G. Bearden;C. Beattie;I. Belikov;A. D. C. Bell Hechavarria;F. Bellini;R. Bellwied;S. Belokurova;V. Belyaev;G. Bencedi;S. Beole;A. Bercuci;Y. Berdnikov;A. Berdnikova;D. Berenyi;L. Bergmann;M. G. Besoiu;L. Betev;P. P. Bhaduri;A. Bhasin;I. R. Bhat;M. A. Bhat;B. Bhattacharjee;P. Bhattacharya;L. Bianchi;N. Bianchi;J. Biel????k;J. Biel????kov??;J. Biernat;A. Bilandzic;G. Biro;S. Biswas;J. T. Blair;D. Blau;M. B. Blidaru;C. Blume;G. Boca;F. Bock;A. Bogdanov;S. Boi;J. Bok;L. Boldizs??r;A. Bolozdynya;M. Bombara;P. M. Bond;G. Bonomi;H. Borel;A. Borissov;H. Bossi;E. Botta;L. Bratrud;P. Braun-Munzinger;M. Bregant;M. Broz;G. E. Bruno;M. D. Buckland;D. Budnikov;H. Buesching;S. Bufalino;O. Bugnon;P. Buhler;Z. Buthelezi;J. B. Butt;S. A. Bysiak;D. Caffarri;M. Cai;H. Caines;A. Caliva;E. Calvo Villar;J. M. M. Camacho;R. S. Camacho;P. Camerini;F. D. M. Canedo;F. Carnesecchi;R. Caron;J. Castillo Castellanos;E. A. R. Casula;F. Catalano;C. Ceballos Sanchez;P. Chakraborty;S. Chandra;S. Chapeland;M. Chartier;S. Chattopadhyay;S. Chattopadhyay;A. Chauvin;T. G. Chavez;C. Cheshkov;B. Cheynis;V. Chibante Barroso;D. D. Chinellato;S. Cho;P. 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2022
Abstract
The production of K∗ (892) 0 and φ(1020) mesons in proton–proton (pp) and lead–lead (Pb–Pb) collisions at √s NN = 5.02 TeV has been measured using the ALICE detector at the Large Hadron Collider (LHC). The transverse momentum (pT ) distributions of K∗ (892) 0 and φ(1020) mesons have been measured at midrapidity (|y| < 0.5) up to pT = 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 pT > 8 GeV/c, the RAA 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 RAA values at high pT (>8 GeV/c) for K∗ (892) 0 and φ(1020) mesons are in agreement within uncertainties for √s NN = 5.02 and 2.76 TeV.
S. Acharya, D. Adamov??, A. Adler, J. Adolfsson, G. Aglieri Rinella, M. Agnello, et al. (2022). Production of K*(892)0 and φ(1020) in pp and Pb-Pb collisions at √sNN=5.02 TeV. PHYSICAL REVIEW C, 106(3), 1-20 [10.1103/physrevc.106.034907].
S. Acharya; D. Adamov??; A. Adler; J. Adolfsson; G. Aglieri Rinella; M. Agnello; N. Agrawal; Z. Ahammed; S. Ahmad; S. U. Ahn; I. Ahuja; Z. Akbar; A. A...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/950875
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