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Midrapidity production of pi(+/-), K-+/-, and (<(p))over bar>p measured by the ALICE experiment at the CERN Large Hadron Collider, in Pb-Pb and inelastic pp collisions at root √sNN = 5.02 TeV, is presented. The invariant yields are measured over a wide transverse momentum (p(T)) range from hundreds of MeV/c up to 20 GeV/c. The results in Pb-Pb collisions are presented as a function of the collision centrality, in the range 0-90%. The comparison of the P-T -integrated particle ratios, i.e., proton-to-pion (p/pi) and kaon-to-pion (K/pi) ratios, with similar measurements in Pb-Pb collisions at root √sNN = 2.76 TeV show no significant energy dependence. Blast-wave fits of the p(T) spectra indicate that in the most central collisions radial flow is slightly larger at 5.02 TeV with respect to 2.76 TeV. Particle ratios (p/pi, K/pi) as a function of p(T) show pronounced maxima at p(T) approximate to 3 GeV/c in central Pb-Pb collisions. At high p(T) , particle ratios at 5.02 TeV are similar to those measured in pp collisions at the same energy and in Pb-Pb collisions at root √sNN = 2.76 TeV. Using the pp reference spectra measured at the same collision energy of 5.02 TeV, the nuclear modification factors for the different particle species are derived. Within uncertainties, the nuclear modification factor is particle species independent for high p(T) and compatible with measurements at root √sNN = 2.76 TeV. The results are compared to state-of-the-art model calculations, which are found to describe the observed trends satisfactorily.
S. Acharya, D. Adamová, S. P. Adhya, A. Adler, J. Adolfsson, M. M. Aggarwal, et al. (2020). Production of charged pions, kaons, and (anti-)protons in Pb-Pb and inelastic collisions at √sNN = 5.02 TeV. PHYSICAL REVIEW C, 101(4), 1-27 [10.1103/physrevc.101.044907].
Production of charged pions, kaons, and (anti-)protons in Pb-Pb and inelastic collisions at √sNN = 5.02 TeV
S. Acharya;D. Adamová;S. P. Adhya;A. Adler;J. Adolfsson;M. M. Aggarwal;G. Aglieri Rinella;M. Agnello;N. Agrawal;Z. Ahammed;S. Ahmad;S. U. Ahn;A. Akindinov;M. Al-Turany;S. N. Alam;D. S. D. Albuquerque;D. Aleksandrov;B. Alessandro;H. M. Alfanda;R. Alfaro Molina;B. Ali;Y. Ali;A. Alici;A. Alkin;J. Alme;T. Alt;L. Altenkamper;I. Altsybeev;M. N. Anaam;C. Andrei;D. Andreou;H. A. Andrews;A. Andronic;M. Angeletti;V. Anguelov;C. Anson;T. Antičić;F. Antinori;P. Antonioli;R. Anwar;N. Apadula;L. Aphecetche;H. Appelshäuser;S. Arcelli;R. Arnaldi;M. Arratia;I. C. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;S. Aziz;M. D. Azmi;A. Badalà;Y. W. Baek;S. Bagnasco;X. Bai;R. Bailhache;R. Bala;A. Baldisseri;M. Ball;S. Balouza;R. C. Baral;R. Barbera;L. Barioglio;G. G. Barnaföldi;L. S. Barnby;V. Barret;P. Bartalini;K. Barth;E. Bartsch;F. Baruffaldi;N. Bastid;S. Basu;G. Batigne;B. Batyunya;P. C. Batzing;D. Bauri;J. L. Bazo Alba;I. G. Bearden;C. Bedda;N. K. Behera;I. Belikov;F. Bellini;R. Bellwied;V. Belyaev;G. Bencedi;S. Beole;A. Bercuci;Y. Berdnikov;D. Berenyi;R. A. Bertens;D. Berzano;M. G. Besoiu;L. Betev;A. Bhasin;I. R. Bhat;M. A. Bhat;H. Bhatt;B. Bhattacharjee;A. Bianchi;L. Bianchi;N. Bianchi;J. Bielčík;J. Bielčíková;A. Bilandzic;G. Biro;R. Biswas;S. Biswas;J. T. Blair;D. Blau;C. Blume;G. Boca;F. Bock;A. Bogdanov;L. Boldizsár;A. Bolozdynya;M. Bombara;G. Bonomi;H. Borel;A. Borissov;M. Borri;H. Bossi;E. Botta;L. Bratrud;P. Braun-Munzinger;M. Bregant;T. A. Broker;M. Broz;E. J. Brucken;E. Bruna;G. E. Bruno;M. D. Buckland;D. Budnikov;H. Buesching;S. Bufalino;O. Bugnon;P. Buhler;P. Buncic;Z. Buthelezi;J. B. Butt;J. T. Buxton;S. A. Bysiak;D. Caffarri;A. Caliva;E. Calvo Villar;R. S. Camacho;P. Camerini;A. A. Capon;F. Carnesecchi;R. Caron;J. Castillo Castellanos;A. J. Castro;E. A. R. Casula;F. Catalano;C. Ceballos Sanchez;P. Chakraborty;S. Chandra;B. Chang;W. Chang;S. Chapeland;M. Chartier;S. Chattopadhyay;S. Chattopadhyay;A. Chauvin;C. Cheshkov;B. Cheynis;V. Chibante Barroso;D. D. Chinellato;S. 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Zardoshti;A. Zarochentsev;P. Závada;N. Zaviyalov;H. Zbroszczyk;M. Zhalov;X. Zhang;Z. Zhang;C. Zhao;V. Zherebchevskii;N. Zhigareva;D. Zhou;Y. Zhou;Z. Zhou;J. Zhu;Y. Zhu;A. Zichichi;M. B. Zimmermann;G. Zinovjev;N. Zurlo
2020
Abstract
Midrapidity production of pi(+/-), K-+/-, and (<(p))over bar>p measured by the ALICE experiment at the CERN Large Hadron Collider, in Pb-Pb and inelastic pp collisions at root √sNN = 5.02 TeV, is presented. The invariant yields are measured over a wide transverse momentum (p(T)) range from hundreds of MeV/c up to 20 GeV/c. The results in Pb-Pb collisions are presented as a function of the collision centrality, in the range 0-90%. The comparison of the P-T -integrated particle ratios, i.e., proton-to-pion (p/pi) and kaon-to-pion (K/pi) ratios, with similar measurements in Pb-Pb collisions at root √sNN = 2.76 TeV show no significant energy dependence. Blast-wave fits of the p(T) spectra indicate that in the most central collisions radial flow is slightly larger at 5.02 TeV with respect to 2.76 TeV. Particle ratios (p/pi, K/pi) as a function of p(T) show pronounced maxima at p(T) approximate to 3 GeV/c in central Pb-Pb collisions. At high p(T) , particle ratios at 5.02 TeV are similar to those measured in pp collisions at the same energy and in Pb-Pb collisions at root √sNN = 2.76 TeV. Using the pp reference spectra measured at the same collision energy of 5.02 TeV, the nuclear modification factors for the different particle species are derived. Within uncertainties, the nuclear modification factor is particle species independent for high p(T) and compatible with measurements at root √sNN = 2.76 TeV. The results are compared to state-of-the-art model calculations, which are found to describe the observed trends satisfactorily.
S. Acharya, D. Adamová, S. P. Adhya, A. Adler, J. Adolfsson, M. M. Aggarwal, et al. (2020). Production of charged pions, kaons, and (anti-)protons in Pb-Pb and inelastic collisions at √sNN = 5.02 TeV. PHYSICAL REVIEW C, 101(4), 1-27 [10.1103/physrevc.101.044907].
S. Acharya; D. Adamová; S. P. Adhya; A. Adler; J. Adolfsson; M. M. Aggarwal; G. Aglieri Rinella; M. Agnello; N. Agrawal; Z. Ahammed; S. Ahmad; S. U. A...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/775664
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simulazione ASN
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.
La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.