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The production of prompt D-0, D-s(+) and Lambda(+)(c) hadrons, and their ratios, D-s(+)/D-0 and Lambda(+)(c)/D-0, are measured in proton-proton collisions at root s = 13 TeV at midrapidity (vertical bar y vertical bar < 0.5) with the ALICE detector at the LHC. The measurements are performed as a function of the charm-hadron transverse momentum (p(T)) in intervals of charged-particle multiplicity, measured with two multiplicity estimators covering different pseudorapidity regions. While the strange to non-strange D-s(+)/D-0 ratio indicates no significant multiplicity dependence, the baryon-to-meson P-T-differential Lambda(+)(c)/D-0 ratio shows a multiplicity-dependent enhancement, with a significance of 5.3 sigma for 1 < p(T) < 12 GeV/c, comparing the highest multiplicity interval with respect to the lowest one. The measurements are compared with a theoretical model that explains the multiplicity dependence by a canonical treatment of quantum charges in the statistical hadronisation approach, and with predictions from event generators that implement colour reconnection mechanisms beyond the leading colour approximation to model the hadronisation process. The Lambda(+)(c)/D-0 ratios as a function of p(T) present a similar shape and magnitude as the Lambda/K-s(0) ratios in comparable multiplicity intervals, suggesting a potential common mechanism for light- and charmhadron formation, with analogous multiplicity dependence. The p(T)-integrated ratios, extrapolated down to p(T) = 0, do not show a significant dependence on multiplicity within the uncertainties. (C) 2022 European Organization for Nuclear Research. Published by Elsevier B.V.
Observation of a multiplicity dependence in the pT-differential charm baryon-to-meson ratios in proton–proton collisions at s=13 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;G. Alocco;T. Alt;I. Altsybeev;M. N. Anaam;C. Andrei;D. Andreou;A. Andronic;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;Z. Banoo;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;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;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;M. C. Danisch;A. Danu;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;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;J. Do;A. Dobrin;B. D??nigus;A. K. Dubey;A. Dubla;S. Dudi;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. Eulisse;D. Evans;S. Evdokimov;L. Fabbietti;M. Faggin;J. Faivre;F. Fan;W. Fan;A. Fantoni;M. Fasel;P. Fecchio;A. Feliciello;G. Feofilov;A. Fern??ndez T??llez;A. Ferrero;A. Ferretti;V. J. G. Feuillard;J. Figiel;V. Filova;D. Finogeev;F. M. Fionda;G. Fiorenza;F. Flor;A. N. Flores;S. Foertsch;S. Fokin;E. Fragiacomo;E. Frajna;A. Francisco;U. Fuchs;N. Funicello;C. Furget;A. Furs;J. J. Gaardh??je;M. Gagliardi;A. M. Gago;A. Gal;C. D. Galvan;P. Ganoti;C. Garabatos;J. R. A. Garcia;E. Garcia-Solis;K. Garg;C. Gargiulo;A. Garibli;K. Garner;P. Gasik;E. F. Gauger;A. Gautam;M. B. Gay Ducati;M. Germain;P. Ghosh;S. K. Ghosh;M. Giacalone;P. Gianotti;P. Giubellino;P. Giubilato;A. M. C. Glaenzer;P. Gl??ssel;E. Glimos;D. J. Q. Goh;V. Gonzalez;L. H. Gonz??lez-Trueba;S. Gorbunov;M. Gorgon;L. G??rlich;S. Gotovac;V. Grabski;L. K. Graczykowski;L. Greiner;A. Grelli;C. Grigoras;V. Grigoriev;S. Grigoryan;F. Grosa;J. F. Grosse-Oetringhaus;R. Grosso;D. Grund;G. G. Guardiano;R. Guernane;M. Guilbaud;K. Gulbrandsen;T. Gunji;W. Guo;A. Gupta;R. Gupta;S. P. Guzman;L. Gyulai;M. K. Habib;C. Hadjidakis;H. Hamagaki;M. Hamid;R. Hannigan;M. R. Haque;A. Harlenderova;J. W. Harris;A. Harton;J. A. Hasenbichler;H. Hassan;D. Hatzifotiadou;P. Hauer;L. B. Havener;S. T. Heckel;E. Hellb??r;H. Helstrup;T. Herman;E. G. Hernandez;G. Herrera Corral;F. Herrmann;K. F. Hetland;H. Hillemanns;C. Hills;B. Hippolyte;B. Hofman;B. Hohlweger;J. Honermann;G. H. Hong;D. Horak;S. Hornung;A. Horzyk;R. Hosokawa;Y. Hou;P. Hristov;C. Hughes;P. Huhn;L. M. Huhta;C. V. Hulse;T. J. Humanic;H. Hushnud;L. A. Husova;A. Hutson;J. P. Iddon;R. Ilkaev;H. Ilyas;M. Inaba;G. M. Innocenti;M. Ippolitov;A. Isakov;T. Isidori;M. S. Islam;M. Ivanov;V. Ivanov;V. Izucheev;M. Jablonski;B. Jacak;N. Jacazio;P. M. Jacobs;S. Jadlovska;J. Jadlovsky;S. Jaelani;C. Jahnke;M. J. Jakubowska;A. Jalotra;M. A. Janik;T. Janson;M. Jercic;O. Jevons;A. A. P. Jimenez;F. Jonas;P. G. Jones;J. M. Jowett;J. Jung;M. Jung;A. Junique;A. Jusko;M. J. Kabus;J. Kaewjai;P. Kalinak;A. S. Kalteyer;A. 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Shou;Y. Sibiriak;S. Siddhanta;T. Siemiarczuk;T. F. Silva;D. Silvermyr;T. Simantathammakul;G. Simonetti;B. Singh;R. Singh;R. Singh;R. 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;C. Soncco;J. Song;A. Songmoolnak;F. Soramel;S. Sorensen;I. Sputowska;J. Stachel;I. Stan;P. J. Steffanic;S. F. Stiefelmaier;D. Stocco;I. Storehaug;M. M. Storetvedt;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;A. Szabo;I. Szarka;U. Tabassam;S. F. Taghavi;G. Taillepied;J. Takahashi;G. J. Tambave;S. Tang;Z. Tang;J. D. Tapia Takaki;M. G. Tarzila;A. Tauro;G. Tejeda Mu??oz;A. Telesca;L. Terlizzi;C. Terrevoli;G. Tersimonov;S. Thakur;D. Thomas;R. Tieulent;A. Tikhonov;A. R. Timmins;M. Tkacik;A. Toia;N. Topilskaya;M. Toppi;F. Torales-Acosta;T. Tork;A. Trifir??;S. Tripathy;T. Tripathy;S. Trogolo;V. Trubnikov;W. H. Trzaska;T. P. Trzcinski;A. Tumkin;R. 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Zherebchevskii;Y. Zhi;N. Zhigareva;D. Zhou;Y. Zhou;J. Zhu;Y. Zhu;G. Zinovjev;N. Zurlo
2022-01-01
Abstract
The production of prompt D-0, D-s(+) and Lambda(+)(c) hadrons, and their ratios, D-s(+)/D-0 and Lambda(+)(c)/D-0, are measured in proton-proton collisions at root s = 13 TeV at midrapidity (vertical bar y vertical bar < 0.5) with the ALICE detector at the LHC. The measurements are performed as a function of the charm-hadron transverse momentum (p(T)) in intervals of charged-particle multiplicity, measured with two multiplicity estimators covering different pseudorapidity regions. While the strange to non-strange D-s(+)/D-0 ratio indicates no significant multiplicity dependence, the baryon-to-meson P-T-differential Lambda(+)(c)/D-0 ratio shows a multiplicity-dependent enhancement, with a significance of 5.3 sigma for 1 < p(T) < 12 GeV/c, comparing the highest multiplicity interval with respect to the lowest one. The measurements are compared with a theoretical model that explains the multiplicity dependence by a canonical treatment of quantum charges in the statistical hadronisation approach, and with predictions from event generators that implement colour reconnection mechanisms beyond the leading colour approximation to model the hadronisation process. The Lambda(+)(c)/D-0 ratios as a function of p(T) present a similar shape and magnitude as the Lambda/K-s(0) ratios in comparable multiplicity intervals, suggesting a potential common mechanism for light- and charmhadron formation, with analogous multiplicity dependence. The p(T)-integrated ratios, extrapolated down to p(T) = 0, do not show a significant dependence on multiplicity within the uncertainties. (C) 2022 European Organization for Nuclear Research. Published by Elsevier B.V.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.11769/549244
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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.