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Abstract: The production of π±, K±, and ( p )p is measured in pp collisions at √s = 13 TeV
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, RT = NT/〈NT〉, 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 〈NT〉 is the mean value over all the analysed events. The first measurements
of identified particle pT spectra as a function of RT in the three topological regions are
reported. It is found that the yield of high transverse momentum particles relative to the
RT-integrated measurement decreases with increasing RT in both the toward and the away
regions, indicating that the softer UE dominates particle production as RT increases and
validating that RT 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 )/(π+ + π−) and (K+ + K−)/(π+ + π−) in
the low UE limit (RT → 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.
Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at $$ \sqrt{s} $$ = 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. Chibante Barroso;D. D. Chinellato;E. S. Chizzali;J. Cho;S. Cho;P. Chochula;P. Christakoglou;C. H. Christensen;P. Christiansen;T. Chujo;M. Ciacco;C. Cicalo;F. Cindolo;M. R. Ciupek;G. Clai;F. Colamaria;J. S. Colburn;D. Colella;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;C. Cot;J. Crkovsk??;P. Crochet;R. Cruz-Torres;E. Cuautle;P. Cui;A. Dainese;M. C. Danisch;A. Danu;P. Das;P. Das;S. Das;A. R. Dash;S. Dash;A. De Caro;G. de Cataldo;J. de Cuveland;A. De Falco;D. De Gruttola;N. De Marco;C. De Martin;S. De Pasquale;S. Deb;R. J. Debski;K. R. Deja;R. Del Grande;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;A. Dobrin;B. D??nigus;J. M. 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. 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Gunji;W. Guo;A. Gupta;R. Gupta;S. P. Guzman;L. Gyulai;M. K. Habib;C. Hadjidakis;F. U. Haider;H. Hamagaki;A. Hamdi;M. Hamid;Y. Han;R. Hannigan;M. R. Haque;J. W. Harris;A. Harton;H. Hassan;D. Hatzifotiadou;P. Hauer;L. B. Havener;S. T. Heckel;E. Hellb??r;H. Helstrup;M. Hemmer;T. Herman;G. Herrera Corral;F. Herrmann;S. Herrmann;K. F. Hetland;B. Heybeck;H. Hillemanns;C. Hills;B. Hippolyte;F. W. Hoffmann;B. Hofman;B. Hohlweger;G. H. Hong;M. Horst;A. Horzyk;R. Hosokawa;Y. Hou;P. Hristov;C. Hughes;P. Huhn;L. M. Huhta;C. V. Hulse;T. J. Humanic;A. Hutson;D. Hutter;J. P. Iddon;R. Ilkaev;H. Ilyas;M. Inaba;G. M. Innocenti;M. Ippolitov;A. Isakov;T. Isidori;M. S. Islam;M. Ivanov;M. Ivanov;V. Ivanov;M. Jablonski;B. Jacak;N. Jacazio;P. M. Jacobs;S. Jadlovska;J. Jadlovsky;S. Jaelani;L. Jaffe;C. Jahnke;M. J. Jakubowska;M. A. Janik;T. Janson;M. Jercic;S. Jia;A. A. P. Jimenez;F. Jonas;J. M. Jowett;J. Jung;M. Jung;A. Junique;A. Jusko;M. J. Kabus;J. Kaewjai;P. Kalinak;A. S. Kalteyer;A. Kalweit;V. Kaplin;A. Karasu Uysal;D. Karatovic;O. Karavichev;T. Karavicheva;P. Karczmarczyk;E. Karpechev;U. Kebschull;R. Keidel;D. L. D. Keijdener;M. Keil;B. Ketzer;A. M. Khan;S. Khan;A. Khanzadeev;Y. Kharlov;A. Khatun;A. Khuntia;M. B. Kidson;B. Kileng;B. Kim;C. Kim;D. J. Kim;E. J. Kim;J. Kim;J. S. Kim;J. Kim;M. Kim;S. Kim;T. Kim;K. Kimura;S. Kirsch;I. Kisel;S. Kiselev;A. Kisiel;J. P. Kitowski;J. L. Klay;J. Klein;S. Klein;C. Klein-B??sing;M. Kleiner;T. Klemenz;A. Kluge;A. G. Knospe;C. Kobdaj;T. Kollegger;A. Kondratyev;N. Kondratyeva;E. Kondratyuk;J. Konig;S. A. Konigstorfer;P. J. Konopka;G. Kornakov;S. D. Koryciak;A. Kotliarov;V. Kovalenko;M. Kowalski;V. Kozhuharov;I. Kr??lik;A. Krav????kov??;L. Kreis;M. Krivda;F. Krizek;K. Krizkova Gajdosova;M. Kroesen;M. Kr??ger;D. M. Krupova;E. Kryshen;V. Ku??era;C. Kuhn;P. G. Kuijer;T. Kumaoka;D. Kumar;L. Kumar;N. Kumar;S. Kumar;S. Kundu;P. Kurashvili;A. Kurepin;A. B. Kurepin;A. Kuryakin;S. Kushpil;J. Kvapil;M. J. Kweon;J. Y. Kwon;Y. Kwon;S. L. La Pointe;P. La Rocca;Y. S. Lai;A. Lakrathok;M. Lamanna;R. Langoy;P. Larionov;E. Laudi;L. Lautner;R. Lavicka;T. Lazareva;R. Lea;H. Lee;G. Legras;J. Lehrbach;R. C. Lemmon;I. Le??n Monz??n;M. M. Lesch;E. D. Lesser;M. Lettrich;P. L??vai;X. Li;X. L. Li;J. Lien;R. Lietava;I. Likmeta;B. Lim;S. H. Lim;V. Lindenstruth;A. Lindner;C. Lippmann;A. Liu;D. H. Liu;J. Liu;I. M. Lofnes;C. Loizides;S. Lokos;J. Lomker;P. Loncar;J. A. Lopez;X. Lopez;E. L??pez Torres;P. Lu;J. R. Luhder;M. Lunardon;G. Luparello;Y. G. Ma;A. Maevskaya;M. Mager;T. Mahmoud;A. Maire;M. V. Makariev;M. Malaev;G. Malfattore;N. M. Malik;Q. W. Malik;S. K. Malik;L. Malinina;D. Mal???Kevich;D. Mallick;N. Mallick;G. Mandaglio;V. Manko;F. Manso;V. Manzari;Y. Mao;G. V. Margagliotti;A. Margotti;A. Mar??n;C. Markert;P. Martinengo;J. L. Martinez;M. I. Mart??nez;G. Mart??nez Garc??a;S. Masciocchi;M. Masera;A. Masoni;L. Massacrier;A. Mastroserio;O. Matonoha;P. F. T. Matuoka;A. Matyja;C. Mayer;A. L. Mazuecos;F. Mazzaschi;M. Mazzilli;J. E. Mdhluli;A. F. 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Sharma;S. Sharma;U. Sharma;A. Shatat;O. Sheibani;K. Shigaki;M. Shimomura;J. Shin;S. Shirinkin;Q. Shou;Y. Sibiriak;S. Siddhanta;T. Siemiarczuk;T. F. Silva;D. Silvermyr;T. Simantathammakul;R. Simeonov;B. Singh;B. Singh;R. Singh;R. Singh;R. Singh;S. Singh;V. K. Singh;V. Singhal;T. Sinha;B. Sitar;M. Sitta;T. B. Skaali;G. Skorodumovs;M. Slupecki;N. Smirnov;R. J. M. Snellings;E. H. Solheim;J. Song;A. Songmoolnak;F. Soramel;R. Spijkers;I. Sputowska;J. Staa;J. Stachel;I. Stan;P. J. Steffanic;S. F. Stiefelmaier;D. Stocco;I. Storehaug;P. Stratmann;S. Strazzi;C. P. Stylianidis;A. A. P. Suaide;C. Suire;M. Sukhanov;M. Suljic;R. Sultanov;V. Sumberia;S. Sumowidagdo;S. Swain;I. Szarka;M. Szymkowski;S. F. Taghavi;G. Taillepied;J. Takahashi;G. J. Tambave;S. Tang;Z. Tang;J. D. Tapia Takaki;N. Tapus;L. A. Tarasovicova;M. G. Tarzila;G. F. Tassielli;A. Tauro;G. Tejeda Mu??oz;A. Telesca;L. Terlizzi;C. Terrevoli;G. Tersimonov;S. Thakur;D. Thomas;A. Tikhonov;A. R. Timmins;M. Tkacik;T. Tkacik;A. Toia;R. Tokumoto;N. Topilskaya;M. Toppi;F. Torales-Acosta;T. Tork;A. G. Torres Ramos;A. Trifir??;A. S. Triolo;S. Tripathy;T. Tripathy;S. Trogolo;V. Trubnikov;W. H. Trzaska;T. P. Trzcinski;A. Tumkin;R. Turrisi;T. S. Tveter;K. Ullaland;B. Ulukutlu;A. Uras;M. Urioni;G. L. Usai;M. Vala;N. Valle;L. V. R. van Doremalen;M. van Leeuwen;C. A. van Veen;R. J. G. van Weelden;P. Vande Vyvre;D. Varga;Z. Varga;M. Vasileiou;A. Vasiliev;O. V??zquez Doce;V. Vechernin;E. Vercellin;S. Vergara Lim??n;L. Vermunt;R. V??rtesi;M. Verweij;L. Vickovic;Z. Vilakazi;O. Villalobos Baillie;A. Villani;G. Vino;A. Vinogradov;T. Virgili;V. Vislavicius;A. Vodopyanov;B. Volkel;M. A. V??lkl;K. Voloshin;S. A. Voloshin;G. Volpe;B. von Haller;I. Vorobyev;N. Vozniuk;J. Vrl??kov??;C. Wang;D. Wang;Y. Wang;A. Wegrzynek;F. T. Weiglhofer;S. C. Wenzel;J. P. Wessels;S. L. Weyhmiller;J. Wiechula;J. Wikne;G. Wilk;J. Wilkinson;G. A. Willems;B. Windelband;M. Winn;J. R. Wright;W. Wu;Y. Wu;R. Xu;A. Yadav;A. K. Yadav;S. Yalcin;Y. Yamaguchi;S. Yang;S. Yano;Z. Yin;I. -K. Yoo;J. H. Yoon;S. Yuan;A. Yuncu;V. Zaccolo;C. Zampolli;F. Zanone;N. Zardoshti;A. Zarochentsev;P. Z??vada;N. Zaviyalov;M. Zhalov;B. Zhang;L. Zhang;S. Zhang;X. Zhang;Y. Zhang;Z. Zhang;M. Zhao;V. Zherebchevskii;Y. Zhi;D. Zhou;Y. Zhou;J. Zhu;Y. Zhu;S. C. Zugravel;N. Zurlo
2023-01-01
Abstract
Abstract: The production of π±, K±, and ( p )p is measured in pp collisions at √s = 13 TeV
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, RT = NT/〈NT〉, 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 〈NT〉 is the mean value over all the analysed events. The first measurements
of identified particle pT spectra as a function of RT in the three topological regions are
reported. It is found that the yield of high transverse momentum particles relative to the
RT-integrated measurement decreases with increasing RT in both the toward and the away
regions, indicating that the softer UE dominates particle production as RT increases and
validating that RT 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 )/(π+ + π−) and (K+ + K−)/(π+ + π−) in
the low UE limit (RT → 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.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11579/159302
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