In ultraperipheral collisions (UPCs) of relativistic nuclei without overlap of nuclear densities, the two nuclei are excited by the Lorentz-contracted Coulomb fields of their collision partners. In these UPCs, the typical nuclear excitation energy is below a few tens of MeV, and a small number of nucleons are emitted in electromagnetic dissociation (EMD) of primary nuclei, in contrast to complete nuclear fragmentation in hadronic interactions. The cross sections of emission of given numbers of neutrons in UPCs of 208Pb nuclei at & RADIC;sNN = 5.02 TeV were measured with the neutron zero degree calorimeters (ZDCs) of the ALICE detector at the LHC, exploiting a similar technique to that used in previous studies performed at & RADIC;sNN = 2.76 TeV. In addition, the cross sections for the exclusive emission of one, two, three, four, and five forward neutrons in the EMD, not accompanied by the emission of forward protons, and thus mostly corresponding to the production of 207,206,205,204,203Pb, respectively, were measured for the first time. The predictions from the available models describe the measured cross sections well. These cross sections can be used for evaluating the impact of secondary nuclei on the LHC components, in particular, on superconducting magnets, and also provide useful input for the design of the Future Circular Collider (FCC-hh).
Neutron emission in ultraperipheral Pb-Pb collisions at √sNN=5.02 TeV / Acharya, S; Adamová, D; Adler, A; Adolfsson, J; Aggarwal, Mm; Rinella, Ga; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, Su; Akindinov, A; Al-Turany, M; Alam, Sn; Albuquerque, Dsd; Aleksandrov, D; Alessandro, B; Alfanda, Hm; Molina, Ra; Ali, B; Ali, Y; Alici, A; Alkin, A; Alme, J; Alt, T; Altenkamper, L; Altsybeev, I; Anaam, Mn; Andrei, C; Andreou, D; Andrews, Ha; Andronic, A; Angeletti, M; Anguelov, V; Anson, C; Anticic, T; Antinori, F; Antonioli, P; Anwar, R; Apadula, N; Aphecetche, L; Appelshaeuser, H; Arcelli, S; Arnaldi, R; Arratia, M; Arsene, Ic; Arslandok, M; Augustinus, A; Averbeck, R; Aziz, S; Azmi, Md; Badala, A; Baek, Yw; Bagnasco, S; Bai, X; Bailhache, R; Bala, R; Baldisseri, A; Ball, M; Balouza, S; Barbera, R; Barioglio, L; Barnafoldi, Gg; Barnby, Ls; Barret, V; Bartalini, P; Barth, K; Bartsch, E; Baruffaldi, F; Bastid, N; Basu, S; Batigne, G; Batyunya, B; Bauri, D; Alba, Jlb; Bearden, Ig; Bedda, C; Behera, Nk; Belikov, I; Hechavarria, Adcb; Bellini, F; Bellwied, R; Belyaev, V; Bencedi, G; Beole, S; Bercuci, A; Berdnikov, Y; Berenyi, D; Bertens, Ra; Berzano, D; Besoiu, Mg; Betev, L; Bhasin, A; Bhat, Ir; Bhat, Ma; Bhatt, H; Bhattacharjee, B; Bianchi, A; Bianchi, L; Bianchi, N; Bielcík, J; Bielcíková, J; Bilandzic, A; Biro, G; Biswas, R; Biswas, S; Blair, Jt; Blau, D; Blume, C; Boca, G; Bock, F; Bogdanov, A; Boi, S; Boldizsár, L; Bolozdynya, A; Bombara, M; Bonomi, G; Borel, H; Borissov, A; Bossi, H; Botta, E; Bratrud, L; Braun-Munzinger, P; Bregant, M; Broz, M; Brucken, J; Bruna, E; Bruno, Ge; Buckland, Md; Budnikov, D; Buesching, H; Bufalino, S; Bugnon, O; Buhler, P; Buncic, P; Buthelezi, Z; Butt, Jb; Buxton, Jt; Bysiak, Sa; Caffarri, D; Caliva, A; Villar, Ec; Camacho, Rs; Camerini, P; Capon, Aa; Carnesecchi, F; Caron, R; Castellanos, Jc; Castro, Aj; Casula, Ear; Catalano, F; Sanchez, Cc; Chakraborty, P; Chandra, S; Chang, W; Chapeland, S; Chartier, M; Chattopadhyay, S; Chattopadhyay, S; Chauvin, A; Cheshkov, C; Cheynis, B; Barroso, Vc; Chinellato, Dd; Cho, S; Chochula, P; Chowdhury, T; Christakoglou, P; Christensen, Ch; Christiansen, P; Chujo, T; Cicalo, C; Cifarelli, L; Cindolo, F; Cleymans, J; Colamaria, F; Colella, D; Collu, A; Colocci, M; Concas, M; Balbastre, Gc; del Valle, Zc; Contin, G; Contreras, Jg; Cormier, Tm; Morales, Yc; Cortese, P; Cosentino, Mr; Costa, F; Costanza, S; Crochet, P; Cuautle, E; Cui, P; Cunqueiro, L; Dabrowski, D; Dahms, T; Dainese, A; Damas, Fpa; Danisch, Mc; Danu, A; Das, D; Das, I; Das, P; Das, P; Das, S; Dash, A; Dash, S; De, S; De Caro, A; de Cataldo, G; de Cuveland, J; De Falco, A; De Gruttola, D; De Marco, N; De Pasquale, S; Deb, S; Debjani, B; Degenhardt, Hf; Deja, Kr; Deloff, A; Delsanto, S; Devetak, D; Dhankher, P; Di Bari, D; Di Mauro, A; Diaz, Ra; Dietel, T; Dillenseger, P; Ding, Y; Diviá, R; Dixit, Du; Djuvsland, O; Dmitrieva, U; Dobrin, A; Dönigus, B; Dordic, O; Dubey, Ak; Dubla, A; Dudi, S; Dukhishyam, M; Dupieux, P; Ehlers, Rj; 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[10.1103/PhysRevC.107.064902]
Neutron emission in ultraperipheral Pb-Pb collisions at √sNN=5.02 TeV
Acharya, S; Adamová, D; Adler, A; Adolfsson, J; Aggarwal, MM; Rinella, GA; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, SU; Akindinov, A; Al-Turany, M; Alam, SN; Albuquerque, DSD; Aleksandrov, D; Alessandro, B; Alfanda, HM; Molina, RA; Ali, B; Ali, Y; Alici, A; Alkin, A; Alme, J; Alt, T; Altenkamper, L; Altsybeev, I; Anaam, MN; Andrei, C; Andreou, D; Andrews, HA; Andronic, A; Angeletti, M; Anguelov, V; Anson, C; Anticic, T; Antinori, F; Antonioli, P; Anwar, R; Apadula, N; Aphecetche, L; Appelshaeuser, H; Arcelli, S; Arnaldi, R; Arratia, M; Arsene, IC; Arslandok, M; Augustinus, A; Averbeck, R; Aziz, S; Azmi, MD; Badala, A; Baek, YW; Bagnasco, S; Bai, X; Bailhache, R; Bala, R; Baldisseri, A; Ball, M; Balouza, S; Barbera, R; Barioglio, L; Barnafoldi, GG; Barnby, LS; Barret, V; Bartalini, P; Barth, K; Bartsch, E; Baruffaldi, F; Bastid, N; Basu, S; Batigne, G; Batyunya, B; Bauri, D; Alba, JLB; Bearden, IG; Bedda, C; Behera, NK; Belikov, I; Hechavarria, ADCB; Bellini, F; Bellwied, R; Belyaev, V; 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Zhou, Z; Zhu, J; Zhu, Y; Zichichi, A; Zimmermann, MB; Zinovjev, G; Zurlo, N
2023-01-01
Abstract
In ultraperipheral collisions (UPCs) of relativistic nuclei without overlap of nuclear densities, the two nuclei are excited by the Lorentz-contracted Coulomb fields of their collision partners. In these UPCs, the typical nuclear excitation energy is below a few tens of MeV, and a small number of nucleons are emitted in electromagnetic dissociation (EMD) of primary nuclei, in contrast to complete nuclear fragmentation in hadronic interactions. The cross sections of emission of given numbers of neutrons in UPCs of 208Pb nuclei at & RADIC;sNN = 5.02 TeV were measured with the neutron zero degree calorimeters (ZDCs) of the ALICE detector at the LHC, exploiting a similar technique to that used in previous studies performed at & RADIC;sNN = 2.76 TeV. In addition, the cross sections for the exclusive emission of one, two, three, four, and five forward neutrons in the EMD, not accompanied by the emission of forward protons, and thus mostly corresponding to the production of 207,206,205,204,203Pb, respectively, were measured for the first time. The predictions from the available models describe the measured cross sections well. These cross sections can be used for evaluating the impact of secondary nuclei on the LHC components, in particular, on superconducting magnets, and also provide useful input for the design of the Future Circular Collider (FCC-hh).
Citazione
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[10.1103/PhysRevC.107.064902]
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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.