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: The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of _{Λ}^{3}H in p-Pb collisions at sqrt[s_{NN}]=5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval -1<0 for the 40% highest-multiplicity p-Pb collisions is dN/dy=[6.3±1.8(stat)±1.2(syst)]×10^{-7}. The measurement is compared with the expectations of statistical hadronization and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in charged particle multiplicity environments relevant to small collision systems such as p-Pb, and therefore the measurement of dN/dy is crucial to distinguish between them. The precision of this measurement leads to the exclusion with a significance larger than 6.9σ of some configurations of the statistical hadronization model, thus constraining the theory behind the production of loosely bound states at hadron colliders.
Hypertriton Production in p-Pb Collisions at sqrt[s_{NN}]=5.02 TeV
Acharya, S;Adamová, D;Adler, A;Aglieri Rinella, G;Agnello, M;Agrawal, N;Ahammed, Z;Ahmad, S;Ahn, S U;Ahuja, I;Akbar, Z;Akindinov, A;Al-Turany, M;Alam, S N;Aleksandrov, D;Alessandro, B;Alfanda, H M;Alfaro Molina, R;Ali, B;Ali, Y;Alici, A;Alizadehvandchali, N;Alkin, A;Alme, J;Alt, T;Altenkamper, L;Altsybeev, I;Anaam, M N;Andrei, C;Andreou, D;Andronic, A;Angeletti, M;Anguelov, V;Antinori, F;Antonioli, P;Anuj, C;Apadula, N;Aphecetche, L;Appelshäuser, H;Arcelli, S;Arnaldi, R;Arsene, I C;Arslandok, M;Augustinus, A;Averbeck, R;Aziz, S;Azmi, M D;Badalà, A;Baek, Y W;Bai, X;Bailhache, R;Bailung, Y;Bala, R;Balbino, A;Baldisseri, A;Balis, B;Ball, M;Banerjee, D;Barbera, R;Barioglio, L;Barlou, M;Barnaföldi, G G;Barnby, L S;Barret, V;Bartels, C;Barth, K;Bartsch, E;Baruffaldi, F;Bastid, N;Basu, S;Batigne, G;Batyunya, B;Bauri, D;Bazo Alba, J L;Bearden, I G;Beattie, C;Belikov, I;Bell Hechavarria, A D C;Bellini, F;Bellwied, R;Belokurova, S;Belyaev, V;Bencedi, G;Beole, S;Bercuci, A;Berdnikov, Y;Berdnikova, A;Bergmann, L;Besoiu, M G;Betev, L;Bhaduri, P P;Bhasin, A;Bhat, I R;Bhat, M A;Bhattacharjee, B;Bhattacharya, P;Bianchi, L;Bianchi, N;Bielčík, J;Bielčíková, J;Biernat, J;Bilandzic, A;Biro, G;Biswas, S;Blair, J T;Blau, D;Blidaru, M B;Blume, C;Boca, G;Bock, F;Bogdanov, A;Boi, S;Bok, J;Boldizsár, L;Bolozdynya, A;Bombara, M;Bond, P M;Bonomi, G;Borel, H;Borissov, A;Bossi, H;Botta, E;Bratrud, L;Braun-Munzinger, P;Bregant, M;Broz, M;Bruno, G E;Buckland, M D;Budnikov, D;Buesching, H;Bufalino, S;Bugnon, O;Buhler, P;Buthelezi, Z;Butt, J B;Bysiak, S A;Cai, M;Caines, H;Caliva, A;Calvo Villar, E;Camacho, J M M;Camacho, R S;Camerini, P;Canedo, F D M;Carnesecchi, F;Caron, R;Castillo Castellanos, J;Casula, E A R;Catalano, F;Ceballos Sanchez, C;Chakraborty, P;Chandra, S;Chapeland, S;Chartier, M;Chattopadhyay, S;Chattopadhyay, S;Chauvin, A;Chavez, T G;Cheng, T;Cheshkov, C;Cheynis, B;Chibante Barroso, V;Chinellato, D D;Cho, S;Chochula, P;Christakoglou, P;Christensen, C H;Christiansen, P;Chujo, T;Cicalo, C;Cifarelli, L;Cindolo, F;Ciupek, M R;Clai, G;Cleymans, J;Colamaria, F;Colburn, J S;Colella, D;Collu, A;Colocci, M;Concas, M;Conesa Balbastre, G;Conesa Del Valle, Z;Contin, G;Contreras, J G;Coquet, M L;Cormier, T M;Cortese, P;Cosentino, M R;Costa, F;Costanza, S;Crochet, P;Cruz-Torres, R;Cuautle, E;Cui, P;Cunqueiro, L;Dainese, A;Danisch, M C;Danu, A;Das, I;Das, P;Das, P;Das, S;Dash, S;De, S;De Caro, A;de Cataldo, G;De Cilladi, L;de Cuveland, J;De Falco, A;De Gruttola, D;De Marco, N;De Martin, C;De Pasquale, S;Deb, S;Degenhardt, H F;Deja, K R;Dello Stritto, L;Delsanto, S;Deng, W;Dhankher, P;Di Bari, D;Di Mauro, A;Diaz, R A;Dietel, T;Ding, Y;Divià, R;Dixit, D U;Djuvsland, Ø;Dmitrieva, U;Do, J;Dobrin, A;Dönigus, B;Dordic, O;Dubey, A K;Dubla, A;Dudi, S;Dukhishyam, M;Dupieux, P;Dzalaiova, N;Eder, T M;Ehlers, R J;Eikeland, V N;Eisenhut, F;Elia, D;Erazmus, B;Ercolessi, F;Erhardt, F;Erokhin, A;Ersdal, M R;Espagnon, B;Eulisse, G;Evans, D;Evdokimov, S;Fabbietti, L;Faggin, 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E;Kazantsev, A;Kebschull, U;Keidel, R;Keijdener, D L D;Keil, M;Ketzer, B;Khabanova, Z;Khan, A M;Khan, S;Khanzadeev, A;Kharlov, Y;Khatun, A;Khuntia, A;Kileng, B;Kim, B;Kim, C;Kim, D J;Kim, E J;Kim, J;Kim, J S;Kim, J;Kim, J;Kim, J;Kim, M;Kim, S;Kim, T;Kirsch, S;Kisel, I;Kiselev, S;Kisiel, A;Kitowski, J P;Klay, J L;Klein, J;Klein, S;Klein-Bösing, C;Kleiner, M;Klemenz, T;Kluge, A;Knospe, A G;Kobdaj, C;Köhler, M K;Kollegger, T;Kondratyev, A;Kondratyeva, N;Kondratyuk, E;Konig, J;Konigstorfer, S A;Konopka, P J;Kornakov, G;Koryciak, S D;Koska, L;Kotliarov, A;Kovalenko, O;Kovalenko, V;Kowalski, M;Králik, I;Kravčáková, A;Kreis, L;Krivda, M;Krizek, F;Krizkova Gajdosova, K;Kroesen, M;Krüger, M;Kryshen, E;Krzewicki, M;Kučera, V;Kuhn, C;Kuijer, P G;Kumaoka, T;Kumar, D;Kumar, L;Kumar, N;Kundu, S;Kurashvili, P;Kurepin, A;Kurepin, A B;Kuryakin, A;Kushpil, S;Kvapil, J;Kweon, M J;Kwon, J Y;Kwon, Y;La Pointe, S L;La Rocca, P;Lai, Y S;Lakrathok, A;Lamanna, M;Langoy, R;Lapidus, K;Larionov, P;Laudi, E;Lautner, L;Lavicka, R;Lazareva, T;Lea, R;Lehrbach, J;Lemmon, R C;León Monzón, I;Lesser, E D;Lettrich, M;Lévai, P;Li, X;Li, X L;Lien, J;Lietava, R;Lim, B;Lim, S H;Lindenstruth, V;Lindner, A;Lippmann, C;Liu, A;Liu, D H;Liu, J;Lofnes, I M;Loginov, V;Loizides, C;Loncar, P;Lopez, J A;Lopez, X;López Torres, E;Luhder, J R;Lunardon, M;Luparello, G;Ma, Y G;Maevskaya, A;Mager, M;Mahmoud, T;Maire, A;Malaev, M;Malik, N M;Malik, Q W;Malinina, L;Mal'Kevich, D;Mallick, N;Malzacher, P;Mandaglio, G;Manko, V;Manso, F;Manzari, V;Mao, Y;Mareš, J;Margagliotti, G V;Margotti, A;Marín, A;Markert, C;Marquard, M;Martin, N A;Martinengo, P;Martinez, J L;Martínez, M I;Martínez García, G;Masciocchi, S;Masera, M;Masoni, A;Massacrier, L;Mastroserio, A;Mathis, A M;Matonoha, O;Matuoka, P F T;Matyja, A;Mayer, C;Mazuecos, A L;Mazzaschi, F;Mazzilli, M;Mazzoni, M A;Mdhluli, J E;Mechler, A F;Meddi, F;Melikyan, Y;Menchaca-Rocha, A;Meninno, E;Menon, A S;Meres, M;Mhlanga, S;Miake, Y;Micheletti, L;Migliorin, L C;Mihaylov, D 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H;Peresunko, D;Perez, G M;Perrin, S;Pestov, Y;Petráček, V;Petrovici, M;Pezzi, R P;Piano, S;Pikna, M;Pillot, P;Pinazza, O;Pinsky, L;Pinto, C;Pisano, S;Płoskoń, M;Planinic, M;Pliquett, F;Poghosyan, M G;Polichtchouk, B;Politano, S;Poljak, N;Pop, A;Porteboeuf-Houssais, S;Porter, J;Pozdniakov, V;Prasad, S K;Preghenella, R;Prino, F;Pruneau, C A;Pshenichnov, I;Puccio, M;Qiu, S;Quaglia, L;Quishpe, R E;Ragoni, S;Rakotozafindrabe, A;Ramello, L;Rami, F;Ramirez, S A R;Ramos, A G T;Rancien, T A;Raniwala, R;Raniwala, S;Räsänen, S S;Rath, R;Ravasenga, I;Read, K F;Redelbach, A R;Redlich, K;Rehman, A;Reichelt, P;Reidt, F;Reme-Ness, H A;Renfordt, R;Rescakova, Z;Reygers, K;Riabov, A;Riabov, V;Richert, T;Richter, M;Riegler, W;Riggi, F;Ristea, C;Rodríguez Cahuantzi, M;Røed, K;Rogalev, R;Rogochaya, E;Rogoschinski, T S;Rohr, D;Röhrich, D;Rojas, P F;Rokita, P S;Ronchetti, F;Rosano, A;Rosas, E D;Rossi, A;Rotondi, A;Roy, A;Roy, P;Roy, S;Rubini, N;Rueda, O V;Rui, R;Rumyantsev, B;Russek, P G;Rustamov, 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2022-01-01
Abstract
: The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of _{Λ}^{3}H in p-Pb collisions at sqrt[s_{NN}]=5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval -1<0 for the 40% highest-multiplicity p-Pb collisions is dN/dy=[6.3±1.8(stat)±1.2(syst)]×10^{-7}. The measurement is compared with the expectations of statistical hadronization and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in charged particle multiplicity environments relevant to small collision systems such as p-Pb, and therefore the measurement of dN/dy is crucial to distinguish between them. The precision of this measurement leads to the exclusion with a significance larger than 6.9σ of some configurations of the statistical hadronization model, thus constraining the theory behind the production of loosely bound states at hadron colliders.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/1889741
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simulazione ASN
Il report seguente simula gli indicatori relativi alla produzione scientifica in relazione alle soglie ASN 2018-2020 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 presenta gli indicatori calcolati alla data indicata sul report. Si ricorda che in sede di domanda ASN presso il MIUR gli indicatori saranno invece calcolati a partire dal 1° gennaio rispettivamente del quinto/decimo/quindicesimo anno precedente la scadenza del quadrimestre di presentazione della domanda (art 2 del DM 598/2018).
In questa simulazione pertanto il valore degli indicatori potrà differire da quello conteggiato all’atto della domanda ASN effettuata presso il MIUR a seguito di:
Correzioni imputabili a eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori.
Presenza di eventuali errori di catalogazione e/o dati mancanti in IRIS
Variabilità nel tempo dei valori citazionali (per i settori bibliometrici)
Variabilità della finestra temporale considerata in funzione della sessione di domanda ASN a cui si partecipa.
La presente simulazione è stata realizzata sulla base delle regole riportate nel DM 598/2018 e dell'allegata Tabella A e delle specifiche definite all'interno del Focus Group Cineca relativo al modulo IRIS ER. Il Cineca non si assume alcuna responsabilità in merito all'uso che il diretto interessato o terzi faranno della simulazione.