K∗(892)0 and φ(1020) production in p-Pb collisions at √sNN = 8.16 TeV
dc.contributor.author | ALICE Collaboration | |
dc.date.accessioned | 2023-07-07T12:45:50Z | |
dc.date.available | 2023-07-07T12:45:50Z | |
dc.date.issued | 2023 | |
dc.identifier.citation | ALICE Collaboration. (2023). K∗(892)0 and φ(1020) production in p-Pb collisions at √sNN = 8.16 TeV. <i>Physical Review C</i>, <i>107</i>(5), Article 055201. <a href="https://doi.org/10.1103/PhysRevC.107.055201" target="_blank">https://doi.org/10.1103/PhysRevC.107.055201</a> | |
dc.identifier.other | CONVID_183824199 | |
dc.identifier.uri | https://jyx.jyu.fi/handle/123456789/88322 | |
dc.description.abstract | The production of K∗(892)0 and ϕ(1020)resonances has been measured in p-Pb collisions at √sNN = 8.16 TeV using the ALICE detector. Resonances are reconstructed via their hadronic decay channels in the rapidity interval −0.5 < y < 0 and the transverse momentum spectra are measured for various multiplicity classes up to pT = 20 GeV/c for K∗(892)0and pT = 16 GeV/c for ϕ(1020). The pT-integrated yields and mean transverse momenta are reported and compared with previous results in pp, p-Pb and Pb-Pb collisions. The xT scaling for K∗(892)0and ϕ(1020)resonance production is newly tested in p-Pb collisions and found to hold in the high-pT region at Large Hadron Collider energies. The nuclear modification factors (RpPb) as a function of pT for K*0 and ϕ at √sNN = 8.16 TeV are presented along with the new RpPb measurements of K*0, ϕ, Ξ, and Ω at √sNN = 5.02 TeV. At intermediate pT (2–8 GeV/c), RpPb of Ξ, Ω show a Cronin-like enhancement, while K*0 and ϕ show no or little nuclear modification. At high pT (>8 GeV/c), the RpPb values of all hadrons are consistent with unity within uncertainties. The RpPb of K∗(892)0and ϕ(1020)at √sNN = 8.16 and 5.02 TeV show no significant energy dependence. | en |
dc.format.mimetype | application/pdf | |
dc.language.iso | eng | |
dc.publisher | American Physical Society (APS) | |
dc.relation.ispartofseries | Physical Review C | |
dc.rights | CC BY 4.0 | |
dc.title | K∗(892)0 and φ(1020) production in p-Pb collisions at √sNN = 8.16 TeV | |
dc.type | article | |
dc.identifier.urn | URN:NBN:fi:jyu-202307074449 | |
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 | 2469-9985 | |
dc.relation.numberinseries | 5 | |
dc.relation.volume | 107 | |
dc.type.version | publishedVersion | |
dc.rights.copyright | ©2023 CERN, for the ALICE Collaboration | |
dc.rights.accesslevel | openAccess | fi |
dc.subject.yso | ydinfysiikka | |
dc.subject.yso | hadronit | |
dc.format.content | fulltext | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p14759 | |
jyx.subject.uri | http://www.yso.fi/onto/yso/p39838 | |
dc.rights.url | https://creativecommons.org/licenses/by/4.0/ | |
dc.relation.doi | 10.1103/PhysRevC.107.055201 | |
dc.type.okm | A1 |