Multi-strange baryon production at mid-rapidity in Pb-Pb collisions at root s(NN)=2.76 TeV
dc.contributor.author | ALICE Collaboration | |
dc.date.accessioned | 2014-12-15T10:47:44Z | |
dc.date.available | 2014-12-15T10:47:44Z | |
dc.date.issued | 2014 | |
dc.identifier.citation | ALICE Collaboration. (2014). Multi-strange baryon production at mid-rapidity in Pb-Pb collisions at root s(NN)=2.76 TeV. <i>Physics Letters B</i>, <i>728</i>(January), 216-227. <a href="https://doi.org/10.1016/j.physletb.2013.11.048" target="_blank">https://doi.org/10.1016/j.physletb.2013.11.048</a> | |
dc.identifier.other | CONVID_23764764 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/44883 | |
dc.description.abstract | The production of − and − baryons and their anti-particles in Pb–Pb collisions at √sNN = 2.76 TeV has been measured using the ALICE detector. The transverse momentum spectra at mid-rapidity (|y| < 0.5) for charged and hyperons have been studied in the range 0.6 < pT < 8.0 GeV/c and 1.2 < pT < 7.0 GeV/c, respectively, and in several centrality intervals (from the most central 0–10% to the most peripheral 60–80% collisions). These spectra have been compared with the predictions of recent hydrodynamic models. In particular, the Kraków and EPOS models give a satisfactory description of the data, with the latter covering a wider pT range. Mid-rapidity yields, integrated over pT, have been determined. The hyperon-to-pion ratios are similar to those at RHIC: they rise smoothly with centrality up to Npart ∼ 150 and saturate thereafter. The enhancements (yields per participant nucleon relative to those in pp collisions) increase both with the strangeness content of the baryon and with centrality, but are less pronounced than at lower energies. | |
dc.language.iso | eng | |
dc.publisher | Elsevier BV * North-Holland | |
dc.relation.ispartofseries | Physics Letters B | |
dc.subject.other | proton-proton collisions | |
dc.title | Multi-strange baryon production at mid-rapidity in Pb-Pb collisions at root s(NN)=2.76 TeV | |
dc.type | research article | |
dc.identifier.urn | URN:NBN:fi:jyu-201409262873 | |
dc.contributor.laitos | Fysiikan laitos | fi |
dc.contributor.laitos | Department of Physics | en |
dc.contributor.oppiaine | Fysiikka | fi |
dc.contributor.oppiaine | Physics | en |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | |
dc.date.updated | 2014-09-26T03:30:11Z | |
dc.type.coar | http://purl.org/coar/resource_type/c_2df8fbb1 | |
dc.description.reviewstatus | peerReviewed | |
dc.format.pagerange | 216–227 | |
dc.relation.issn | 0370-2693 | |
dc.relation.numberinseries | January | |
dc.relation.volume | 728 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | © 2013 The Authors. Published by Elsevier B.V. This is an Open Access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work in properly cited. The Creative Commons Public Domain Dedication waiver applies to the data made available in this article, unless otherwise stated. | |
dc.rights.accesslevel | openAccess | fi |
dc.type.publication | article | |
dc.subject.yso | kvarkki-gluoniplasma | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p38826 | |
dc.rights.url | http://creativecommons.org/licenses/by/3.0/ | |
dc.relation.doi | 10.1016/j.physletb.2013.11.048 | |
dc.type.okm | A1 |
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Ellei muuten mainita, aineiston lisenssi on © 2013 The Authors. Published by Elsevier B.V. This is an Open Access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work in properly cited. The Creative Commons Public Domain Dedication waiver applies to the data made available in this article, unless otherwise stated.