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The production yields of non-prompt $\mathrm{D_s}^{+}$ mesons, namely
$\mathrm{D_s}^{+}$ mesons from beauty-hadron decays, were measured for the
first time as a function of the transverse momentum ($p_{\rm T}$) at
midrapidity ($|y|<0.5$) in central and semi-central Pb$-$Pb collisions at a
centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV with the
ALICE experiment at the LHC. The $\mathrm{D_s}^{+}$ mesons and their charge
conjugates were reconstructed from the hadronic decay channel $\mathrm{D_s}^{+}
\to \phi\pi^+$, with $\phi \to {\rm K}^-{\rm K}^+$, in the $4 < p_{\rm T}<36$
GeV/$c$ and $2 < p_{\rm T}<24$ GeV/$c$ intervals for the 0$-$10% and 30$-$50%
centrality classes, respectively. The measured yields of non-prompt
$\mathrm{D_s}^{+}$ mesons are compared to those of prompt $\mathrm{D_s}^{+}$
and non-prompt $\mathrm{D^0}$ mesons by calculating the ratios of the
production yields in Pb$-$Pb collisions and the nuclear modification factor
$R_\mathrm{AA}$. The ratio between the $R_\mathrm{AA}$ of non-prompt
$\mathrm{D_s}^{+}$ and prompt $\mathrm{D_s}^{+}$ mesons, and that between the
$R_\mathrm{AA}$ of non-prompt $\mathrm{D_s}^{+}$ and non-prompt $\mathrm{D^0}$
mesons in central Pb$-$Pb collisions are found to be on average higher than
unity in the $4< p_{\rm T}<12$ GeV/$c$ interval with a statistical significance
of about $1.6\,\sigma$ and $1.7\,\sigma$, respectively. The measured
$R_\mathrm{AA}$ ratios are compared with the predictions of theoretical models
of heavy-quark transport in a hydrodynamically expanding QGP that incorporate
hadronisation via quark recombination.
Measurement of beauty-strange meson production in Pb–Pb collisions at √sNN = 5.02 TeV via non-prompt D+s mesons / Acharya, S., Adamová, D., Adler, A., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahmad, S., Ahn, S.U., Ahuja, I., Akindinov, A., Al-Turany, M., Aleksandrov, D., Alessandro, B., Alfanda, H.M., Alfaro Molina, R., Ali, B., Ali, Y., Alici, A., Alizadehvandchali, N., et al.. - In: PHYSICS LETTERS. SECTION B. - ISSN 0370-2693. - STAMPA. - 846:(2023), pp. 1-16. [10.1016/j.physletb.2022.137561]
Measurement of beauty-strange meson production in Pb–Pb collisions at √sNN = 5.02 TeV via non-prompt D+s mesons
S. Acharya;D. Adamová;A. Adler;G. Aglieri Rinella;M. Agnello;N. Agrawal;Z. Ahammed;S. Ahmad;S. U. Ahn;I. Ahuja;A. Akindinov;M. Al-Turany;D. Aleksandrov;B. Alessandro;H. M. Alfanda;R. Alfaro Molina;B. Ali;Y. Ali;A. Alici;N. Alizadehvandchali;A. Alkin;J. Alme;G. Alocco;T. Alt;I. Altsybeev;M. N. Anaam;C. Andrei;A. Andronic;V. Anguelov;F. Antinori;P. Antonioli;C. Anuj;N. Apadula;L. Aphecetche;H. Appelshäuser;S. Arcelli;R. Arnaldi;I. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;S. Aziz;M. D. Azmi;A. Badalà;Y. W. Baek;X. Bai;R. Bailhache;Y. Bailung;R. Bala;A. Balbino;A. Baldisseri;B. Balis;D. Banerjee;Z. Banoo;R. Barbera;L. Barioglio;M. Barlou;G. G. Barnaföldi;L. S. Barnby;V. Barret;L. Barreto;C. Bartels;K. Barth;E. Bartsch;F. Baruffaldi;N. Bastid;S. Basu;G. Batigne;D. Battistini;B. Batyunya;D. Bauri;J. L. Bazo Alba;I. G. Bearden;C. Beattie;P. Becht;D. Behera;I. Belikov;A. B. Bell Hechavarria;F. Bellini;R. Bellwied;S. Belokurova;V. Belyaev;G. Bencédi;S. Beole;A. Bercuci;Y. Berdnikov;A. Berdnikova;L. Bergmann;M. G. Besoiu;L. Betev;P. Bhaduri;A. Bhasin;I. Bhat;M. A. Bhat;B. Bhattacharjee;L. Bianchi;N. Bianchi;J. Bielčík;J. Bielčíková;J. Biernat;A. Bilandzic;G. Biro;S. Biswas;J. T. Blair;D. Blau;M. B. Blidaru;N. Bluhme;C. Blume;G. Boca;F. Bock;T. Bodova;A. Bogdanov;S. Boi;J. Bok;L. Boldizsár;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. Bruno;M. D. Buckland;D. Budnikov;H. Buesching;S. Bufalino;O. Bugnon;P. Buhler;Z. Buthelezi;J. B. Butt;A. Bylinkin;S. A. Bysiak;M. Cai;H. Caines;A. Caliva;E. Calvo Villar;J. Camacho;P. Camerini;F. Canedo;M. Cărăbaş;F. Carnesecchi;R. Caron;J. Castillo Castellanos;F. Catalano;C. Ceballos Sanchez;I. Chakaberia;P. Chakraborty;S. Chandra;S. Chapeland;M. Chartier;S. Chattopadhyay;S. Chattopadhyay;T. G. Chavez;T. Cheng;C. Cheshkov;B. Cheynis;V. Chibante Barroso;D. Chinellato;E. Chizzali;J. Cho;S. Cho;P. Chochula;P. Christakoglou;C. H. Christensen;P. Christiansen;T. Chujo;M. Ciacco;C. Cicalo;L. Cifarelli;F. Cindolo;M. R. Ciupek;G. Clai;F. Colamaria;J. S. Colburn;D. Colella;A. Collu;M. Colocci;M. Concas;G. Conesa Balbastre;Z. Conesa del Valle;G. Contin;J. G. Contreras;M. L. Coquet;T. M. Cormier;P. Cortese;M. R. Cosentino;F. Costa;S. Costanza;P. Crochet;R. Cruz-Torres;E. Cuautle;P. Cui;L. Cunqueiro;A. Dainese;M. C. Danisch;A. Danu;P. Das;P. Das;S. Das;S. Dash;R. David;A. De Caro;G. de Cataldo;L. De Cilladi;J. de Cuveland;A. De Falco;D. De Gruttola;N. De Marco;C. De Martin;S. De Pasquale;S. Deb;H. F. Degenhardt;K. R. Deja;R R Del Grande;L. Dello Stritto;W. Deng;P. Dhankher;D. Di Bari;A. Di Mauro;R. A. Diaz;T. Dietel;Y. Ding;R. Divià;D. Dixit;Ø. Djuvsland;U. Dmitrieva;A. Dobrin;B. Dönigus;A. K. Dubey;J. Dubinski;A. Dubla;S. Dudi;P. Dupieux;M. Durkac;N. Dzalaiova;T. M. Eder;R. J. Ehlers;V. N. Eikeland;F. Eisenhut;D. Elia;B. Erazmus;F. Ercolessi;F. Erhardt;M. R. Ersdal;B. Espagnon;G. Eulisse;D. Evans;S. Evdokimov;L. Fabbietti;M. 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2023
Abstract
The production yields of non-prompt $\mathrm{D_s}^{+}$ mesons, namely
$\mathrm{D_s}^{+}$ mesons from beauty-hadron decays, were measured for the
first time as a function of the transverse momentum ($p_{\rm T}$) at
midrapidity ($|y|<0.5$) in central and semi-central Pb$-$Pb collisions at a
centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}}=5.02$ TeV with the
ALICE experiment at the LHC. The $\mathrm{D_s}^{+}$ mesons and their charge
conjugates were reconstructed from the hadronic decay channel $\mathrm{D_s}^{+}
\to \phi\pi^+$, with $\phi \to {\rm K}^-{\rm K}^+$, in the $4 < p_{\rm T}<36$
GeV/$c$ and $2 < p_{\rm T}<24$ GeV/$c$ intervals for the 0$-$10% and 30$-$50%
centrality classes, respectively. The measured yields of non-prompt
$\mathrm{D_s}^{+}$ mesons are compared to those of prompt $\mathrm{D_s}^{+}$
and non-prompt $\mathrm{D^0}$ mesons by calculating the ratios of the
production yields in Pb$-$Pb collisions and the nuclear modification factor
$R_\mathrm{AA}$. The ratio between the $R_\mathrm{AA}$ of non-prompt
$\mathrm{D_s}^{+}$ and prompt $\mathrm{D_s}^{+}$ mesons, and that between the
$R_\mathrm{AA}$ of non-prompt $\mathrm{D_s}^{+}$ and non-prompt $\mathrm{D^0}$
mesons in central Pb$-$Pb collisions are found to be on average higher than
unity in the $4< p_{\rm T}<12$ GeV/$c$ interval with a statistical significance
of about $1.6\,\sigma$ and $1.7\,\sigma$, respectively. The measured
$R_\mathrm{AA}$ ratios are compared with the predictions of theoretical models
of heavy-quark transport in a hydrodynamically expanding QGP that incorporate
hadronisation via quark recombination.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11583/2990263
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