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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. Christakoglou;C. H. Christensen;P. Christiansen;T. Chujo;C. Cicalo;L. Cifarelli;F. Cindolo;M. R. Ciupek;G. Clai;J. Cleymans;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;F. P. A. Damas;M. C. Danisch;A. Danu;I. Das;P. Das;P. Das;S. Das;S. Dash;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;L. Dello Stritto;W. Deng;P. Dhankher;D. Di Bari;A. Di Mauro;R. A. Diaz;T. Dietel;Y. Ding;R. Divi??;D. U. Dixit;??. Djuvsland;U. Dmitrieva;J. Do;A. Dobrin;B. D??nigus;A. K. Dubey;A. Dubla;S. Dudi;M. Dukhishyam;P. Dupieux;N. Dzalaiova;T. M. Eder;R. J. Ehlers;V. N. Eikeland;F. Eisenhut;D. Elia;B. Erazmus;F. Ercolessi;F. Erhardt;A. Erokhin;M. R. Ersdal;B. Espagnon;G. 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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.
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/2318/1911270
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simulazione ASN
Il report seguente simula gli indicatori relativi alla 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 presenta gli indicatori calcolati alla data indicata sul report. Si ricorda che in sede di domanda ASN presso il MIUR gli indicatori saranno invece calcolati a partire dal 1° gennaio rispettivamente del quinto/decimo/quindicesimo anno precedente la scadenza del quadrimestre di presentazione della domanda (art 2 del DM 598/2018).
In questa simulazione pertanto il valore degli indicatori potrà differire da quello conteggiato all’atto della domanda ASN effettuata presso il MIUR a seguito di:
Correzioni imputabili a eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori.
Presenza di eventuali errori di catalogazione e/o dati mancanti in IRIS
Variabilità nel tempo dei valori citazionali (per i settori bibliometrici)
Variabilità della finestra temporale considerata in funzione della sessione di domanda ASN a cui si partecipa.
La presente simulazione è stata realizzata sulla base delle regole riportate nel DM 598/2018 e dell'allegata Tabella A e delle specifiche definite all'interno del Focus Group Cineca relativo al modulo IRIS ER. Il Cineca non si assume alcuna responsabilità in merito all'uso che il diretto interessato o terzi faranno della simulazione.