Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at s $$ \sqrt{s} $$ = 13 TeV and in p–Pb collisions at s NN $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV

Acharya, S.; Adamová, D.; Aglieri Rinella, G.; Agnello, M.; Agrawal, N.; Ahammed, Z.; Ahmad, S.; Ahn, S.; Ahuja, I.; Akindinov, A.; Al-Turany, M.; Aleksandrov, D.; Alessandro, B.; Alfanda, H.; Alfaro Molina, R.; Ali, B.; Alici, A.; Alizadehvandchali, N.; Alkin, A.; Alme, J.; Alocco, G.; Alt, T.; Altamura, A.; Altsybeev, I.; Alvarado, J.; Anaam, M.; Andrei, C.; Andreou, N.; Andronic, A.; Anguelov, V.; Antinori, F.; Antonioli, P.; Apadula, N.; Aphecetche, L.; Appelshäuser, H.; Arata, C.; Arcelli, S.; Aresti, M.; Arnaldi, R.; Arneiro, J.; Arsene, I.; Arslandok, M.; Augustinus, A.; Averbeck, R.; Azmi, M.; Baba, H.; Badalà, A.; Bae, J.; Baek, Y.; Bai, X.; Bailhache, R.; Bailung, Y.; Balbino, A.; Baldisseri, A.; Balis, B.; Banerjee, D.; Banoo, Z.; Barbera, R.; Barile, F.; Barioglio, L.; Barlou, M.; Barman, B.; Barnaföldi, G.; Barnby, L.; Barret, V.; Barreto, L.; Bartels, C.; Barth, K.; Bartsch, E.; Bastid, N.; Basu, S.; Batigne, G.; Battistini, D.; Batyunya, B.; Bauri, D.; Bazo Alba, J.; Bearden, I.; Beattie, C.; Becht, P.; Behera, D.; Belikov, I.; Bell Hechavarria, A.; Bellini, F.; Bellwied, R.; Belokurova, S.; Beltran, Y.; Bencedi, G.; Beole, S.; Berdnikov, Y.; Berdnikova, A.; Bergmann, L.; Besoiu, M.; Betev, L.; Bhaduri, P.; Bhasin, A.; Bhat, M.; Bhattacharjee, B.; Bianchi, L.; Bianchi, N.; Bielčík, J.; Bielčíková, J.; Biernat, J.; Bigot, A.; Bilandzic, A.; Biro, G.; Biswas, S.; Bize, N.; Blair, J.; Blau, D.; Blidaru, M.; Bluhme, N.; Blume, C.; Boca, G.; Bock, F.; Bodova, T.; Bogdanov, A.; Boi, S.; Bok, J.; Boldizsár, L.; Bombara, M.; Bond, P.; Bonomi, G.; Borel, H.; Borissov, A.; Borquez Carcamo, A.; Bossi, H.; Botta, E.; Bouziani, Y.; Bratrud, L.; Braun-Munzinger, P.; Bregant, M.; Broz, M.; Bruno, G.; Buckland, M.; Budnikov, D.; Buesching, H.; Bufalino, S.; Buhler, P.; Burmasov, N.; Buthelezi, Z.; Bylinkin, A.; Bysiak, S.; Cai, M.; Caines, H.; Caliva, A.; Calvo Villar, E.; Camacho, J.; Camerini, P.; Canedo, F.; Cantway, S.; Carabas, M.; Carballo, A.; Carnesecchi, F.; Caron, R.; Carvalho, L.; Castillo Castellanos, J.; Catalano, F.; Ceballos Sanchez, C.; Chakaberia, I.; Chakraborty, P.; Chandra, S.; Chapeland, S.; Chartier, M.; Chattopadhyay, S.; Chattopadhyay, S.; Cheng, T.; Cheshkov, C.; Cheynis, B.; Chibante Barroso, V.; Chinellato, D.; Chizzali, E.; Cho, J.; Cho, S.; Chochula, P.; Choudhury, D.; Christakoglou, P.; Christensen, C.; Christiansen, P.; Chujo, T.; Ciacco, M.; Cicalo, C.; Cindolo, F.; Ciupek, M.; Clai, G.; Colamaria, F.; Colburn, J.; Colella, D.; Colocci, M.; Concas, M.; Conesa Balbastre, G.; Conesa del Valle, Z.; Contin, G.; Contreras, J.; Coquet, M.; Cortese, P.; Cosentino, M.; Costa, F.; Costanza, S.; Cot, C.; Crkovská, J.; Crochet, P.; Cruz-Torres, R.; Cui, P.; Dainese, A.; Danisch, M.; Danu, A.; Das, P.; Das, P.; Das, S.; Dash, A.; Dash, S.; Caro, A.; Cataldo, G.; Cuveland, J.; Falco, A.; Gruttola, D.; Marco, N.; Martin, C.; Pasquale, S.; Deb, R.; Grande, R.; Stritto, L.; Deng, W.; Dhankher, P.; Bari, D.; Mauro, A.; Diab, B.; Diaz, R.; Dietel, T.; Ding, Y.; Ditzel, J.; Divià, R.; Dixit, D.; Djuvsland, Ø.; Dmitrieva, U.; Dobrin, A.; Dönigus, B.; Dubinski, J.; Dubla, A.; Dudi, S.; Dupieux, P.; Durkac, M.; Dzalaiova, N.; Eder, T.; Ehlers, R.; Eisenhut, F.; Ejima, R.; Elia, D.; Erazmus, B.; Ercolessi, F.; Espagnon, B.; Eulisse, G.; Evans, D.; Evdokimov, S.; Fabbietti, L.; Faggin, M.; Faivre, J.; Fan, F.; Fan, W.; Fantoni, A.; Fasel, M.; Feliciello, A.; Feofilov, G.; Fernández Téllez, A.; Ferrandi, L.; Ferrer, M.; Ferrero, A.; Ferrero, C.; Ferretti, A.; Feuillard, V.; Filova, V.; Finogeev, D.; Fionda, F.; Flatland, E.; Flor, F.; Flores, A.; Foertsch, S.; Fokin, I.; Fokin, S.; Fragiacomo, E.; Frajna, E.; Fuchs, U.; Funicello, N.; Furget, C.; Furs, A.; Fusayasu, T.; Gaardhøje, J.; Gagliardi, M.; Gago, A.; Gahlaut, T.; Galvan, C.; Gangadharan, D.; Ganoti, P.; Garabatos, C.; García Chávez, T.; Garcia-Solis, E.; Gargiulo, C.; Gasik, P.; Gautam, A.; Gay Ducati, M.; Germain, M.; Ghimouz, A.; Ghosh, C.; Giacalone, M.; Gioachin, G.; Giubellino, P.; 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Kondratyev, A.; Kondratyeva, N.; Kondratyuk, E.; Konig, J.; Konigstorfer, S.; Konopka, P.; Kornakov, G.; Korwieser, M.; Koryciak, S.; Kotliarov, A.; Kovalenko, V.; Kowalski, M.; Kozhuharov, V.; Králik, I.; Kravčáková, A.; Krcal, L.; Krivda, M.; Krizek, F.; Krizkova Gajdosova, K.; Kroesen, M.; Krüger, M.; Krupova, D.; Kryshen, E.; Kučera, V.; Kuhn, C.; Kuijer, P.; Kumaoka, T.; Kumar, D.; Kumar, L.; Kumar, N.; Kumar, S.; Kundu, S.; Kurashvili, P.; Kurepin, A.; Kurepin, A.; Kuryakin, A.; Kushpil, S.; Kuskov, V.; Kweon, M.; Kwon, Y.; Pointe, S.; Rocca, P.; Lakrathok, A.; Lamanna, M.; Landou, A.; Langoy, R.; Larionov, P.; Laudi, E.; Lautner, L.; Lavicka, R.; Lea, R.; Lee, H.; Legrand, I.; Legras, G.; Lehrbach, J.; Lelek, T.; Lemmon, R.; León Monzón, I.; Lesch, M.; Lesser, E.; Lévai, P.; Li, X.; Lien, J.; Lietava, R.; Likmeta, I.; Lim, B.; Lim, S.; Lindenstruth, V.; Lindner, A.; Lippmann, C.; Liu, D.; Liu, J.; Liveraro, G.; Lofnes, I.; Loizides, C.; Lokos, S.; Lömker, J.; Loncar, P.; Lopez, X.; 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Munhoz, M.; Munzer, R.; Murakami, H.; Murray, S.; Musa, L.; Musinsky, J.; Myrcha, J.; Naik, B.; Nambrath, A.; Nandi, B.; Nania, R.; Nappi, E.; Nassirpour, A.; Nath, A.; Nattrass, C.; Naydenov, M.; Neagu, A.; Negru, A.; Nekrasova, E.; Nellen, L.; Nepeivoda, R.; Nese, S.; Neskovic, G.; Nicassio, N.; Nielsen, B.; Nielsen, E.; Nikolaev, S.; Nikulin, S.; Nikulin, V.; Noferini, F.; Noh, S.; Nomokonov, P.; Norman, J.; Novitzky, N.; Nowakowski, P.; Nyanin, A.; Nystrand, J.; Ogino, M.; Oh, S.; Ohlson, A.; Okorokov, V.; Oleniacz, J.; Oliveira Da Silva, A.; Onnerstad, A.; Oppedisano, C.; Ortiz Velasquez, A.; Otwinowski, J.; Oya, M.; Oyama, K.; Pachmayer, Y.; Padhan, S.; Pagano, D.; Paić, G.; Paisano-Guzmán, S.; Palasciano, A.; Panebianco, S.; Park, H.; Park, H.; Park, J.; Parkkila, J.; Patley, Y.; Patra, R.; Paul, B.; Pei, H.; Peitzmann, T.; Peng, X.; Pennisi, M.; Perciballi, S.; Peresunko, D.; Perez, G.; Pestov, Y.; Petrov, V.; Petrovici, M.; Pezzi, R.; Piano, S.; Pikna, M.; Pillot, P.; Pinazza, O.; 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doi:10.1007/JHEP03(2024)092
Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at $\sqrt{s}$ $$ \sqrt{s} $$ = 13 TeV and in p–Pb collisions at $\sqrt{s_{NN}}$ $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV

S. Acharya (Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France) ; D. Adamová (Nuclear Physics Institute of the Czech Academy of Sciences, Husinec-Řež, Czech Republic) ; G. Aglieri Rinella (European Organization for Nuclear Research (CERN), Geneva, Switzerland) ; M. Agnello (Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy) ; N. Agrawal (INFN, Sezione di Bologna, Bologna, Italy) ; et al. - Show all 1054 authors
Long- and short-range correlations for pairs of charged particles are studied via two-particle angular correlations in pp collisions at $\sqrt{s}$ $$ \sqrt{s} $$ = 13 TeV and p–Pb collisions at $\sqrt{s_{NN}}$ $$ \sqrt{s_{\textrm{NN}}} $$ = 5.02 TeV. The correlation functions are measured as a function of relative azimuthal angle ∆φ and pseudorapidity separation ∆η for pairs of primary charged particles within the pseudorapidity interval |η| < 0.9 and the transverse-momentum interval 1 < p T < 4 GeV/c. Flow coefficients are extracted for the long-range correlations (1.6 < |∆η| < 1.8) in various high-multiplicity event classes using the low-multiplicity template fit method. The method is used to subtract the enhanced yield of away-side jet fragments in high-multiplicity events. These results show decreasing flow signals toward lower multiplicity events. Furthermore, the flow coefficients for events with hard probes, such as jets or leading particles, do not exhibit any significant changes compared to those obtained from high-multiplicity events without any specific event selection criteria. The results are compared with hydrodynamic-model calculations, and it is found that a better understanding of the initial conditions is necessary to describe the results, particularly for low-multiplicity events.
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          "organization": "Korea Institute of Science and Technology Information"
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      "surname": "Ahn", 
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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    {
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    {
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    {
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    {
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    {
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    {
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    {
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    {
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        {
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          "value": "Universit\u00e9 Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France", 
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        {
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          "value": "Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\u00fcr Schwerionenforschung GmbH, Darmstadt, Germany", 
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          "value": "Lawrence Berkeley National Laboratory, Berkeley, California, United States", 
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    {
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          "value": "Dipartimento di Fisica e Astronomia dell\u2019Universit\u00e0 and Sezione INFN, Bologna, Italy", 
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    {
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          "value": "Technical University of Ko\u0161ice, Ko\u0161ice, Slovak Republic", 
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    {
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        {
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          "value": "Technical University of Ko\u0161ice, Ko\u0161ice, Slovak Republic", 
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    {
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    {
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        {
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    {
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        {
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    {
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        {
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        {
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        {
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        {
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        {
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        {
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    {
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        {
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          "value": "Johann-Wolfgang-Goethe Universit\u00e4t Frankfurt Institut f\u00fcr Informatik, Fachbereich Informatik und Mathematik, Frankfurt, Germany", 
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        {
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    {
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        {
          "country": "Germany", 
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    {
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    {
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        {
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    {
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    {
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    {
      "surname": "Kondratyev", 
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    {
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        {
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        {
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        {
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    {
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        {
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        {
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    {
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      "affiliations": [
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  "titles": [
    {
      "source": "Springer", 
      "title": "Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> </math>  $$ \\sqrt{s} $$  = 13 TeV and in p\u2013Pb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </math>  $$ \\sqrt{s_{\\textrm{NN}}} $$  = 5.02 TeV"
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      "value": "10.1007/JHEP03(2024)092"
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      "page_end": "35", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2024", 
      "artid": "JHEP03(2024)092", 
      "year": 2024, 
      "page_start": "1", 
      "journal_issue": "3"
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    "date": "2024-03-19T09:30:15.261391", 
    "source": "Springer", 
    "method": "Springer", 
    "submission_number": "41e73d40e5d311eeae4696b6a0e1ccbd"
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  "page_nr": [
    35
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  "license": [
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      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2024"
    }
  ], 
  "control_number": "84134", 
  "collaborations": [
    {
      "value": "The ALICE collaboration"
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      "categories": [
        "nucl-ex", 
        "hep-ex"
      ], 
      "value": "2308.16591"
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  "abstracts": [
    {
      "source": "Springer", 
      "value": "Long- and short-range correlations for pairs of charged particles are studied via two-particle angular correlations in pp collisions at   <math> <msqrt> <mi>s</mi> </msqrt> </math>  $$ \\sqrt{s} $$  = 13 TeV and p\u2013Pb collisions at   <math> <msqrt> <msub> <mi>s</mi> <mi>NN</mi> </msub> </msqrt> </math>  $$ \\sqrt{s_{\\textrm{NN}}} $$  = 5.02 TeV. The correlation functions are measured as a function of relative azimuthal angle \u2206\u03c6 and pseudorapidity separation \u2206\u03b7 for pairs of primary charged particles within the pseudorapidity interval |\u03b7| &lt; 0.9 and the transverse-momentum interval 1 &lt; p T &lt; 4 GeV/c. Flow coefficients are extracted for the long-range correlations (1.6 &lt; |\u2206\u03b7| &lt; 1.8) in various high-multiplicity event classes using the low-multiplicity template fit method. The method is used to subtract the enhanced yield of away-side jet fragments in high-multiplicity events. These results show decreasing flow signals toward lower multiplicity events. Furthermore, the flow coefficients for events with hard probes, such as jets or leading particles, do not exhibit any significant changes compared to those obtained from high-multiplicity events without any specific event selection criteria. The results are compared with hydrodynamic-model calculations, and it is found that a better understanding of the initial conditions is necessary to describe the results, particularly for low-multiplicity events."
    }
  ], 
  "imprints": [
    {
      "date": "2024-03-15", 
      "publisher": "Springer"
    }
  ]
}
Published on:: 15 March 2024
Publisher:: Springer
Published in:: Journal of High Energy Physics , Volume 2024 (2024)
Issue 3
Pages 1-35
DOI:: https://doi.org/10.1007/JHEP03(2024)092
arXiv:: 2308.16591
Copyrights:: The Author(s)
Licence:: CC-BY-4.0
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