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The production of pi (+/-), K-+/-, and ((P) over bar )p is measured in pp collisions at √s = 13TeV in different topological regions of the events. Particle transverse momentum (pT) spectra are measured in the "toward", "transverse", and "away" angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, R-T = N-T/< N-T >, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and < N-T > is the mean value over all the analysed events. The first measurements of identified particle p(T) spectra as a function of R-T in the three topological regions are reported. It is found that the yield of high transverse momentum particles relative to the R-T-integrated measurement decreases with increasing R-T in both the toward and the away regions, indicating that the softer UE dominates particle production as RT increases and validating that R-T can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. Finally, it is observed that the pT-differential particle ratios (p + (P) over bar)/( pi(+) + pi(-)) and (K+ + K-)/(pi(+) + K-) in the low UE limit ( R-T -> 0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e(+)e(-) results.
S. Acharya, D. Adamov??, A. Adler, G. Aglieri Rinella, M. Agnello, N. Agrawal, et al. (2023). Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at √s = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2023(6), 0-35 [10.1007/jhep06(2023)027].
Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at √s = 13 TeV
S. Acharya;D. Adamov??;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;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;N. Apadula;L. Aphecetche;H. Appelsh??user;C. Arata;S. Arcelli;M. Aresti;R. Arnaldi;J. G. M. C. A. Arneiro;I. C. Arsene;M. Arslandok;A. Augustinus;R. Averbeck;M. D. Azmi;A. Badal??;J. Bae;Y. W. Baek;X. Bai;R. Bailhache;Y. Bailung;A. Balbino;A. Baldisseri;B. Balis;D. Banerjee;Z. Banoo;R. Barbera;F. Barile;L. Barioglio;M. Barlou;G. G. Barnaf??ldi;L. S. Barnby;V. Barret;L. Barreto;C. Bartels;K. Barth;E. Bartsch;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. 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;M. A. Bhat;B. Bhattacharjee;L. Bianchi;N. Bianchi;J. Biel????k;J. Biel????kov??;J. Biernat;A. P. Bigot;A. Bilandzic;G. Biro;S. Biswas;N. Bize;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. Boldizs??r;A. Bolozdynya;M. Bombara;P. M. Bond;G. Bonomi;H. Borel;A. Borissov;A. G. Borquez Carcamo;H. Bossi;E. Botta;Y. E. M. Bouziani;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;S. A. Bysiak;M. Cai;H. Caines;A. Caliva;E. Calvo Villar;J. M. M. Camacho;P. Camerini;F. D. M. Canedo;M. Carabas;A. A. Carballo;F. Carnesecchi;R. Caron;L. A. D. Carvalho;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. 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2023
Abstract
The production of pi (+/-), K-+/-, and ((P) over bar )p is measured in pp collisions at √s = 13TeV in different topological regions of the events. Particle transverse momentum (pT) spectra are measured in the "toward", "transverse", and "away" angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, R-T = N-T/< N-T >, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and < N-T > is the mean value over all the analysed events. The first measurements of identified particle p(T) spectra as a function of R-T in the three topological regions are reported. It is found that the yield of high transverse momentum particles relative to the R-T-integrated measurement decreases with increasing R-T in both the toward and the away regions, indicating that the softer UE dominates particle production as RT increases and validating that R-T can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. Finally, it is observed that the pT-differential particle ratios (p + (P) over bar)/( pi(+) + pi(-)) and (K+ + K-)/(pi(+) + K-) in the low UE limit ( R-T -> 0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e(+)e(-) results.
S. Acharya, D. Adamov??, A. Adler, G. Aglieri Rinella, M. Agnello, N. Agrawal, et al. (2023). Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at √s = 13 TeV. JOURNAL OF HIGH ENERGY PHYSICS, 2023(6), 0-35 [10.1007/jhep06(2023)027].
S. Acharya; D. Adamov??; A. Adler; G. Aglieri Rinella; M. Agnello; N. Agrawal; Z. Ahammed; S. Ahmad; S. U. Ahn; I. Ahuja; A. Akindinov; M. Al-Turany; ...espandi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/951056
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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.