dc.contributor.author | ALICE collaboration | |
dc.date.accessioned | 2021-12-20T12:36:17Z | |
dc.date.available | 2021-12-20T12:36:17Z | |
dc.date.issued | 2021 | |
dc.identifier.citation | ALICE collaboration. (2021). Anisotropic flow of identified hadrons in Xe-Xe collisions at √sNN = 5.44 TeV. <i>Journal of High Energy Physics</i>, <i>2021</i>(10), Article 152. <a href="https://doi.org/10.1007/JHEP10(2021)152" target="_blank">https://doi.org/10.1007/JHEP10(2021)152</a> | |
dc.identifier.other | CONVID_102927995 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/79062 | |
dc.description.abstract | Measurements of elliptic (v2) and triangular (v3) flow coefficients of π±, K±, p+p¯, K0S, and Λ+Λ¯ obtained with the scalar product method in Xe-Xe collisions at √sNN = 5.44 TeV are presented. The results are obtained in the rapidity range |y| < 0.5 and reported as a function of transverse momentum, pT, for several collision centrality classes. The flow coefficients exhibit a particle mass dependence for pT < 3 GeV/c, while a grouping according to particle type (i.e., meson and baryon) is found at intermediate transverse momenta (3 < pT < 8 GeV/c). The magnitude of the baryon v2 is larger than that of mesons up to pT = 6 GeV/c. The centrality dependence of the shape evolution of the pT-differential v2 is studied for the various hadron species. The v2 coefficients of π±, K±, and p+p¯ are reproduced by MUSIC hydrodynamic calculations coupled to a hadronic cascade model (UrQMD) for pT < 1 GeV/c. A comparison with vn measurements in the corresponding centrality intervals in Pb-Pb collisions at √sNN = 5.02 TeV yields an enhanced v2 in central collisions and diminished value in semicentral collisions. | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | eng | |
dc.publisher | Springer | |
dc.relation.ispartofseries | Journal of High Energy Physics | |
dc.rights | CC BY 4.0 | |
dc.title | Anisotropic flow of identified hadrons in Xe-Xe collisions at √sNN = 5.44 TeV | |
dc.type | article | |
dc.identifier.urn | URN:NBN:fi:jyu-202112206044 | |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Physics | en |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | |
dc.type.coar | http://purl.org/coar/resource_type/c_2df8fbb1 | |
dc.description.reviewstatus | peerReviewed | |
dc.relation.issn | 1126-6708 | |
dc.relation.numberinseries | 10 | |
dc.relation.volume | 2021 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © 2021 CERN | |
dc.rights.accesslevel | openAccess | fi |
dc.subject.yso | ydinfysiikka | |
dc.subject.yso | hiukkasfysiikka | |
dc.subject.yso | kvarkki-gluoniplasma | |
dc.format.content | fulltext | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p14759 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p15576 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p38826 | |
dc.rights.url | https://creativecommons.org/licenses/by/4.0/ | |
dc.relation.doi | 10.1007/JHEP10(2021)152 | |
dc.type.okm | A1 | |