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Acharya, S, Acosta, FT, Adamova, D, Adolfsson, J, Aggarwal, MM, Rinella, G Aglieri, Agnello, M, Agrawal, N, Ahammed, Z, Ahn, SU et al (show 1002 more authors) , Aiola, S, Akindinov, A, Al-Turany, M, Alam, SN, Albuquerque, DSD, Aleksandrov, D, Alessandro, B, Alfaro Molina, R, 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, Arnold, OW, Arsene, IC, Arslandok, M, Audurier, B, Augustinus, A, Averbeck, R, Azmi, MD, Badala, A, Baek, YW, Bagnasco, S, Bailhache, R, Bala, R, Baldisseri, A, Ball, M, Baral, RC, Barbano, AM, Barbera, R, Barile, F, Barioglio, L, Barnafoldi, GG, Barnby, LS, Barret, V, Bartalini, P, Barth, K, Bartsch, E, Bastid, N, Basu, S, Batigne, G, Batyunya, B, Batzing, PC, Bazo Alba, JL, Bearden, IG, Beck, H, Bedda, C, Behera, NK, Belikov, I, Bellini, F, Bello Martinez, H, Bellwied, R, Beltran, LGE, Belyaev, V, Bencedi, G, Beole, S, Bercuci, A, Berdnikov, Y, Berenyi, D, Bertens, RA, Berzano, D, Betev, L, Bhaduri, PP, Bhasin, A, Bhat, IR, Bhatt, H, Bhattacharjee, B, Bhom, J, Bianchi, A, Bianchi, L, Bianchi, N, Bielcik, J, Bielcikova, J, Bilandzic, A, Biro, G, Biswas, R, Biswas, S, Blair, JT, Blau, D, Blume, C, Boca, G, Bock, F, Bogdanov, A, Boldizsar, L, Bombara, M, Bonomi, G, Bonora, M, Borel, H, Borissov, A, Borri, M, Botta, E, Bourjau, C, Bratrud, L, Braun-Munzinger, P, Bregant, M, Broker, TA, Broz, M, Brucken, EJ, Bruna, E, Bruno, GE, Budnikov, D, Buesching, H, Bufalino, S, Buhler, P, Buncic, P, Busch, O, Buthelezi, Z, Butt, JB, Buxton, JT, Cabala, J, Caffarri, D, Caines, H, Caliva, A, Calvo Villar, E, Camacho, RS, Camerini, P, Capon, AA, Carena, F, Carena, W, Carnesecchi, F, Castellanos, J Castillo, Castro, AJ, Casula, EAR, Ceballos Sanchez, C, Chandra, S, Chang, B, Chang, W, Chapeland, S, Chartier, M 
ORCID: 0000-0003-0578-5567, Chattopadhyay, S, Chauvin, A, Cheshkov, C, Cheynis, B, Barroso, V Chibante, Chinellato, DD, Cho, S, Chochula, P, Chowdhury, T, Christakoglou, P, Christensen, CH, Christiansen, P, Chujo, T, Chung, SU, Cicalo, C, Cifarelli, L, Cindolo, F, Cleymans, J, Colamaria, F, Colella, D, Collu, A, Colocci, M, Concas, M, Balbastre, G Conesa, del Valle, Z Conesa, Contreras, JG, Cormier, TM, Morales, Y Corrales, Cortese, P, Cosentino, MR, Costa, F, Costanza, S, Crkovska, J, Crochet, P, Cuautle, E, Cunqueiro, L, Dahms, T, Dainese, A, Dani, S, Danisch, MC, Danu, A, Das, D, Das, I, Das, S, Dash, A, Dash, S, De, S, De Caro, A, de Cataldo, G, de Conti, C, de Cuveland, J, De Falco, A, De Gruttola, D, De Marco, N, De Pasquale, S, De Souza, RD, Degenhardt, HF, Deisting, A, Deloff, A, Delsanto, S, Deplano, C, Dhankher, P, Di Bari, D, Di Mauro, A, Di Ruzza, B, Diaz, RA, Dietel, T, Dillenseger, P, Ding, Y, Divia, R, Djuvsland, O, Dobrin, A, Domenicis Gimenez, D, Doenigus, B, Dordic, 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(2018)
Anisotropic flow of identified particles in Pb-Pb collisions at root s(NN)=5.02 TeV.
JOURNAL OF HIGH ENERGY PHYSICS, 2018 (9).
6-.
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Abstract
<jats:title>A<jats:sc>bstract</jats:sc></jats:title><jats:p>The elliptic (<jats:italic>v</jats:italic><jats:sub>2</jats:sub>), triangular (<jats:italic>v</jats:italic><jats:sub>3</jats:sub>), and quadrangular (<jats:italic>v</jats:italic><jats:sub>4</jats:sub>) flow coefficients of π<jats:sup>±</jats:sup>, K<jats:sup>±</jats:sup>,<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathrm{p}+\overline{\mathrm{p}},\kern0.5em \Lambda +\overline{\Lambda},\kern0.5em {\mathrm{K}}_{\mathrm{S}}^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mover><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>,</mml:mo><mml:mspace /><mml:mi>Λ</mml:mi><mml:mo>+</mml:mo><mml:mover><mml:mi>Λ</mml:mi><mml:mo>¯</mml:mo></mml:mover><mml:mo>,</mml:mo><mml:mspace /><mml:msubsup><mml:mi>K</mml:mi><mml:mi>S</mml:mi><mml:mn>0</mml:mn></mml:msubsup></mml:math></jats:alternatives></jats:inline-formula>, and the<jats:italic>ϕ</jats:italic>-meson are measured in Pb-Pb collisions at<jats:inline-formula><jats:alternatives><jats:tex-math>$$ {\sqrt{s}}_{\mathrm{NN}}=5.02 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:msqrt><mml:mi>s</mml:mi></mml:msqrt><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>5.02</mml:mn></mml:math></jats:alternatives></jats:inline-formula>TeV. Results obtained with the scalar product method are reported for the rapidity range |<jats:italic>y</jats:italic>|<jats:italic><</jats:italic>0.5 as a function of transverse momentum,<jats:italic>p</jats:italic><jats:sub>T</jats:sub>, at different collision centrality intervals between 0–70%, including ultra-central (0–1%) collisions for<jats:italic>π</jats:italic><jats:sup>±</jats:sup>, K<jats:sup>±</jats:sup>, and<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathrm{p}+\overline{\mathrm{p}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mover><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math></jats:alternatives></jats:inline-formula>. For<jats:italic>p</jats:italic><jats:sub>T</jats:sub><jats:italic><</jats:italic>3 GeV<jats:italic>/c</jats:italic>, the flow coefficients exhibit a particle mass dependence. At intermediate transverse momenta (3 <<jats:italic>p</jats:italic><jats:sub>T</jats:sub>< 8–10 GeV/<jats:italic>c</jats:italic>), particles show an approximate grouping according to their type (i.e., mesons and baryons). The<jats:italic>ϕ</jats:italic>-meson<jats:italic>v</jats:italic><jats:sub>2</jats:sub>, which tests both particle mass dependence and type scaling, follows<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathrm{p}+\overline{\mathrm{p}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mover><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math></jats:alternatives></jats:inline-formula><jats:italic>v</jats:italic><jats:sub>2</jats:sub>at low<jats:italic>p</jats:italic><jats:sub>T</jats:sub>and π<jats:sup>±</jats:sup><jats:italic>v</jats:italic><jats:sub>2</jats:sub>at intermediate<jats:italic>p</jats:italic><jats:sub>T</jats:sub>. The evolution of the shape of<jats:italic>v</jats:italic><jats:sub>n</jats:sub>(<jats:italic>p</jats:italic><jats:sub>T</jats:sub>) as a function of centrality and harmonic number<jats:italic>n</jats:italic>is studied for the various particle species. Flow coefficients of<jats:italic>π</jats:italic><jats:sup>±</jats:sup>, K<jats:sup>±</jats:sup>, and<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathrm{p}+\overline{\mathrm{p}} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>p</mml:mi><mml:mo>+</mml:mo><mml:mover><mml:mi>p</mml:mi><mml:mo>¯</mml:mo></mml:mover></mml:math></jats:alternatives></jats:inline-formula>for<jats:italic>p</jats:italic><jats:sub>T</jats:sub>< 3 GeV/<jats:italic>c</jats:italic>are compared to iEBE-VISHNU and MUSIC hydrodynamical calculations coupled to a hadronic cascade model (UrQMD). The iEBE-VISHNU calculations describe the results fairly well for<jats:italic>p</jats:italic><jats:sub>T</jats:sub>< 2.5 GeV/<jats:italic>c</jats:italic>, while MUSIC calculations reproduce the measurements for<jats:italic>p</jats:italic><jats:sub>T</jats:sub>< 1 GeV/<jats:italic>c</jats:italic>. A comparison to<jats:italic>v</jats:italic><jats:sub>n</jats:sub>coefficients measured in Pb-Pb collisions at<jats:inline-formula><jats:alternatives><jats:tex-math>$$ \sqrt{s_{\mathrm{NN}}}=2.76 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>2.76</mml:mn></mml:math></jats:alternatives></jats:inline-formula>TeV is also provided.</jats:p>
Dimensions
Dimensions
