Femtoscopic correlations of nonidentical charged kaons (K+K-) are studied in Pb-Pb collisions at a center-of -mass energy per nucleon-nucleon collision root sNN = 2.76 TeV by ALICE at the CERN Large Hadron Collider. One-dimensional K+K- correlation functions are analyzed in three centrality classes and eight intervals of particle-pair transverse momentum. The LednickATIN SMALL LETTER Y WITH ACUTE and Luboshitz interaction model used in the K+K- analysis includes the final-state Coulomb interactions between kaons and the final-state interaction through a0(980) and f0(980) resonances. The mass of f0(980) and coupling were extracted from the fit to K+K- correlation functions using the femtoscopic technique. The measured mass and width of the f0(980) resonance are consistent with other published measurements. The height of the phi(1020) meson peak present in the K+K- correlation function rapidly decreases with increasing source radius, qualitatively in agreement with an inverse volume dependence. A phenomenological fit to this trend suggests that the phi(1020) meson yield is dominated by particles produced directly from the hadronization of the system. The small fraction subsequently produced by final-state interactions could not be precisely quantified with data presented in this paper and will be assessed in future work.
Investigation of K plus K- interactions via femtoscopy in Pb-Pb collisions at √sNN=2.76 TeV at the CERN Large Hadron Collider / Acharya, S; Adamová, D; Adler, A; Rinella, Ga; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, Su; Ahuja, I; Akindinov, A; Al-Turany, M; Aleksandrov, D; Alessandro, B; Alfanda, Hm; Molina, Ra; Ali, B; Alici, A; Alizadehvandchali, N; Alkin, A; Alme, J; Alocco, G; Alt, T; Altsybeev, I; Anaam, Mn; Andrei, C; Andronic, A; Anguelov, V; Antinori, F; Antonioli, P; Apadula, N; Aphecetche, L; Appelshäuser, H; Arata, C; Arcelli, S; Aresti, M; Arnaldi, R; Arsene, Ic; Arslandok, M; Augustinus, A; Averbeck, R; Azmi, Md; Badalà, A; Bae, J; Baek, Yw; Bai, X; Bailhache, R; Bailung, Y; Balbino, A; Baldisseri, A; Balis, B; Banerjee, D; Banoo, Z; Barbera, R; Barile, F; Barioglio, L; Barlou, M; Barnaföldi, Gg; Barnby, Ls; Barret, V; Barreto, L; Bartels, C; Barth, K; Bartsch, E; Bastid, N; Basu, S; Batigne, G; Battistini, D; Batyunya, B; Bauri, D; Alba, Jlb; Bearden, Ig; Beattie, C; Becht, P; Behera, D; Belikov, I; Hechavarria, Adcb; Bellini, F; Bellwied, R; Belokurova, S; Belyaev, V; Bencedi, G; Beole, S; Bercuci, A; Berdnikov, Y; Berdnikova, A; Bergmann, L; Besoiu, Mg; Betev, L; Bhaduri, Pp; Bhasin, A; Bhat, Ma; Bhattacharjee, B; Bianchi, L; Bianchi, N; Bielcík, J; Bielcíková, J; Biernat, J; Bigot, Ap; Bilandzic, A; Biro, G; Biswas, S; Bize, N; Blair, Jt; Blau, D; Blidaru, Mb; Bluhme, N; Blume, C; Boca, G; Bock, F; Bodova, T; Bogdanov, A; Boi, S; Bok, J; Boldizsár, L; Bolozdynya, A; Bombara, M; Bond, Pm; Bonomi, G; Borel, H; Borissov, A; Bossi, H; Botta, E; Bouziani, Yem; Bratrud, L; Braun-Munzinger, P; Bregant, M; Broz, M; Bruno, Ge; Buckland, Md; Budnikov, D; Buesching, H; Bufalino, S; Bugnon, O; Buhler, P; Buthelezi, Z; Bysiak, Sa; Cai, M; Caines, H; Caliva, A; Villar, Ec; Camacho, Jmm; Camerini, P; Canedo, Fdm; Carabas, M; Carballo, Aa; Carcamo, Agb; Carnesecchi, F; Caron, R; Carvalho, Lad; Castellanos, Jc; Catalano, F; Sanchez, Cc; Chakaberia, I; Chakraborty, P; Chandra, S; Chapeland, S; Chartier, M; Chattopadhyay, S; Chattopadhyay, S; Chavez, Tg; Cheng, T; Cheshkov, C; Cheynis, B; Barroso, Vc; Chinellato, Dd; Chizzali, Es; Cho, J; Cho, S; Chochula, P; Christakoglou, P; Christensen, Ch; Christiansen, P; Chujo, T; Ciacco, M; Cicalo, C; Cindolo, F; Ciupek, Mr; Clai, G; Colamaria, F; Colburn, Js; Colella, D; Colocci, M; Concas, M; Balbastre, Gc; del Valle, Zc; Contin, G; Contreras, Jg; Coquet, Ml; Cormier, Tm; Cortese, P; Cosentino, Mr; Costa, F; Costanza, S; Cot, C; Crkovská, J; Crochet, P; Cruz-Torres, R; Cuautle, E; Cui, P; Dainese, A; Danisch, Mc; Danu, A; Das, P; Das, P; Das, S; Dash, Ar; Dash, S; De Caro, A; de Cataldo, G; de Cuveland, J; De Falco, A; De Gruttola, D; De Marco, N; De Martin, C; De Pasquale, S; Deb, S; Debski, Rj; Deja, Kr; Del Grande, R; Dello Stritto, L; Deng, W; Dhankher, P; Di Bari, D; Di Mauro, A; Diaz, Ra; Dietel, T; Ding, Y; Divià, R; Dixit, Du; Djuvsland, O; Dmitrieva, U; Dobrin, A; Dönigus, B; Dubinski, Jm; Dubla, A; 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[10.1103/PhysRevC.107.054904]
Investigation of K plus K- interactions via femtoscopy in Pb-Pb collisions at √sNN=2.76 TeV at the CERN Large Hadron Collider
Acharya, S; Adamová, D; Adler, A; Rinella, GA; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, SU; Ahuja, I; Akindinov, A; Al-Turany, M; Aleksandrov, D; Alessandro, B; Alfanda, HM; Molina, RA; Ali, B; Alici, A; Alizadehvandchali, N; Alkin, A; Alme, J; Alocco, G; Alt, T; Altsybeev, I; Anaam, MN; Andrei, C; Andronic, A; Anguelov, V; Antinori, F; Antonioli, P; Apadula, N; Aphecetche, L; Appelshäuser, H; Arata, C; Arcelli, S; Aresti, M; Arnaldi, R; Arsene, IC; Arslandok, M; Augustinus, A; Averbeck, R; Azmi, MD; Badalà, A; Bae, J; Baek, YW; Bai, X; Bailhache, R; Bailung, Y; Balbino, A; Baldisseri, A; Balis, B; Banerjee, D; Banoo, Z; Barbera, R; Barile, F; Barioglio, L; Barlou, M; Barnaföldi, GG; Barnby, LS; Barret, V; Barreto, L; Bartels, C; Barth, K; Bartsch, E; Bastid, N; Basu, S; Batigne, G; Battistini, D; Batyunya, B; Bauri, D; Alba, JLB; Bearden, IG; Beattie, C; Becht, P; Behera, D; Belikov, I; Hechavarria, ADCB; Bellini, F; Bellwied, R; Belokurova, S; Belyaev, V; Bencedi, G; Beole, S; Bercuci, A; Berdnikov, Y; Berdnikova, A; Bergmann, L; Besoiu, MG; Betev, L; Bhaduri, PP; Bhasin, A; Bhat, MA; Bhattacharjee, B; Bianchi, L; Bianchi, N; Bielcík, J; Bielcíková, J; Biernat, J; Bigot, AP; Bilandzic, A; Biro, G; Biswas, S; Bize, N; Blair, JT; Blau, D; Blidaru, MB; Bluhme, N; Blume, C; Boca, G; Bock, F; Bodova, T; Bogdanov, A; Boi, S; Bok, J; Boldizsár, L; Bolozdynya, A; Bombara, M; Bond, PM; Bonomi, G; Borel, H; Borissov, A; Bossi, H; Botta, E; Bouziani, YEM; Bratrud, L; Braun-Munzinger, P; Bregant, M; Broz, M; Bruno, GE ;Buckland, MD; Budnikov, D; Buesching, H; Bufalino, S; Bugnon, O; Buhler, P; Buthelezi, Z; Bysiak, SA; Cai, M; Caines, H; Caliva, A; Villar, EC; Camacho, JMM; Camerini, P; Canedo, FDM; Carabas, M; Carballo, AA; Carcamo, AGB; Carnesecchi, F; Caron, R; Carvalho, LAD; Castellanos, JC; Catalano, F; Sanchez, CC; Chakaberia, I; Chakraborty, P; Chandra, S; Chapeland, S; Chartier, M; Chattopadhyay, S; Chattopadhyay, S; Chavez, TG; Cheng, T; Cheshkov, C; Cheynis, B; 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2023-01-01
Abstract
Femtoscopic correlations of nonidentical charged kaons (K+K-) are studied in Pb-Pb collisions at a center-of -mass energy per nucleon-nucleon collision root sNN = 2.76 TeV by ALICE at the CERN Large Hadron Collider. One-dimensional K+K- correlation functions are analyzed in three centrality classes and eight intervals of particle-pair transverse momentum. The LednickATIN SMALL LETTER Y WITH ACUTE and Luboshitz interaction model used in the K+K- analysis includes the final-state Coulomb interactions between kaons and the final-state interaction through a0(980) and f0(980) resonances. The mass of f0(980) and coupling were extracted from the fit to K+K- correlation functions using the femtoscopic technique. The measured mass and width of the f0(980) resonance are consistent with other published measurements. The height of the phi(1020) meson peak present in the K+K- correlation function rapidly decreases with increasing source radius, qualitatively in agreement with an inverse volume dependence. A phenomenological fit to this trend suggests that the phi(1020) meson yield is dominated by particles produced directly from the hadronization of the system. The small fraction subsequently produced by final-state interactions could not be precisely quantified with data presented in this paper and will be assessed in future work.
Citazione
Investigation of K plus K- interactions via femtoscopy in Pb-Pb collisions at √sNN=2.76 TeV at the CERN Large Hadron Collider / Acharya, S; Adamová, D; Adler, A; Rinella, Ga; Agnello, M; Agrawal, N; Ahammed, Z; Ahmad, S; Ahn, Su; Ahuja, I; Akindinov, A; Al-Turany, M; Aleksandrov, D; Alessandro, B; Alfanda, Hm; Molina, Ra; Ali, B; Alici, A; Alizadehvandchali, N; Alkin, A; Alme, J; Alocco, G; Alt, T; Altsybeev, I; Anaam, Mn; Andrei, C; Andronic, A; Anguelov, V; Antinori, F; Antonioli, P; Apadula, N; Aphecetche, L; Appelshäuser, H; Arata, C; Arcelli, S; Aresti, M; Arnaldi, R; Arsene, Ic; Arslandok, M; Augustinus, A; Averbeck, R; Azmi, Md; Badalà, A; Bae, J; Baek, Yw; Bai, X; Bailhache, R; Bailung, Y; Balbino, A; Baldisseri, A; Balis, B; Banerjee, D; Banoo, Z; Barbera, R; Barile, F; Barioglio, L; Barlou, M; Barnaföldi, Gg; Barnby, Ls; Barret, V; Barreto, L; Bartels, C; Barth, K; Bartsch, E; Bastid, N; Basu, S; Batigne, G; Battistini, D; Batyunya, B; Bauri, D; Alba, Jlb; Bearden, Ig; Beattie, C; 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[10.1103/PhysRevC.107.054904]
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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.