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This article reports on the inclusive production cross section of several quarkonium states, J/psi, psi(2S), Upsilon(1S), Upsilon(2S), and Upsilon(3S), measured with the ALICE detector at the LHC, in pp collisions at root s = 5.02 TeV. The analysis is performed in the dimuon decay channel at forward rapidity (2.5 < y < 4). The integrated cross sections and transverse-momentum (p(T)) and rapidity (y) differential cross sections for J/psi, psi(2S), Upsilon(1S), and the psi(2S)-to-J/psi cross section ratios are presented. The integrated cross sections, assuming unpolarized quarkonia, are: sigma(J/psi) (p(T) < 20 GeV/c) = 5.88 +/- 0.03 +/- 0.34 mu b, sigma(psi(2S)) (p(T) < 12 GeV/c) = 0.87 +/- 0.06 +/- 0.10 mu b, sigma(Upsilon(1S)) (p(T) < 15 GeV/c) = 45.5 +/- 3.9 +/- 3.5 nb, sigma(Upsilon(2S)) (p(T) < 15 GeV/c) = 22.4 +/- 3.2 +/- 2.7 nb, and sigma(Upsilon(3S)) (p(T) < 15 GeV/c) = 4.9 +/- 2.2 +/- 1.0 nb, where the first (second) uncertainty is the statistical (systematic) one. For the first time, the cross sections of the three Upsilon states, as well as the psi(2S) one as a function of p(T) and y, are measured at root s = 5.02 TeV at forward rapidity. These measurements also significantly extend the J/psi p(T) reach and supersede previously published results. A comparison with ALICE measurements in pp collisions at root s = 2.76, 7, 8, and 13 TeV is presented and the energy dependence of quarkonium production cross sections is discussed. Finally, the results are compared with the predictions from several production models.
Inclusive quarkonium production in pp collisions at $$\sqrt{s}$$ = 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;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;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;P. Becht;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;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;A. Bylinkin;S. A. Bysiak;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;T. Cheng;C. Cheshkov;B. Cheynis;V. Chibante Barroso;D. D. Chinellato;S. Cho;P. Chochula;P. 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Zhi;N. Zhigareva;D. Zhou;Y. Zhou;J. Zhu;Y. Zhu;G. Zinovjev;N. Zurlo
2023-01-01
Abstract
This article reports on the inclusive production cross section of several quarkonium states, J/psi, psi(2S), Upsilon(1S), Upsilon(2S), and Upsilon(3S), measured with the ALICE detector at the LHC, in pp collisions at root s = 5.02 TeV. The analysis is performed in the dimuon decay channel at forward rapidity (2.5 < y < 4). The integrated cross sections and transverse-momentum (p(T)) and rapidity (y) differential cross sections for J/psi, psi(2S), Upsilon(1S), and the psi(2S)-to-J/psi cross section ratios are presented. The integrated cross sections, assuming unpolarized quarkonia, are: sigma(J/psi) (p(T) < 20 GeV/c) = 5.88 +/- 0.03 +/- 0.34 mu b, sigma(psi(2S)) (p(T) < 12 GeV/c) = 0.87 +/- 0.06 +/- 0.10 mu b, sigma(Upsilon(1S)) (p(T) < 15 GeV/c) = 45.5 +/- 3.9 +/- 3.5 nb, sigma(Upsilon(2S)) (p(T) < 15 GeV/c) = 22.4 +/- 3.2 +/- 2.7 nb, and sigma(Upsilon(3S)) (p(T) < 15 GeV/c) = 4.9 +/- 2.2 +/- 1.0 nb, where the first (second) uncertainty is the statistical (systematic) one. For the first time, the cross sections of the three Upsilon states, as well as the psi(2S) one as a function of p(T) and y, are measured at root s = 5.02 TeV at forward rapidity. These measurements also significantly extend the J/psi p(T) reach and supersede previously published results. A comparison with ALICE measurements in pp collisions at root s = 2.76, 7, 8, and 13 TeV is presented and the energy dependence of quarkonium production cross sections is discussed. Finally, the results are compared with the predictions from several production models.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11379/572566
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande.
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