Näytä suppeat kuvailutiedot

dc.contributor.authorALICE Collaboration
dc.date.accessioned2024-03-15T14:19:58Z
dc.date.available2024-03-15T14:19:58Z
dc.date.issued2023
dc.identifier.citationALICE Collaboration. (2023). Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at √ s = 13 TeV. <i>Physical Review D</i>, <i>108</i>(11), Article 112003. <a href="https://doi.org/10.1103/PhysRevD.108.112003" target="_blank">https://doi.org/10.1103/PhysRevD.108.112003</a>
dc.identifier.otherCONVID_207580554
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/93951
dc.description.abstractThe production cross sections of D0 and Λ+c hadrons originating from beauty-hadron decays (i.e., nonprompt) were measured for the first time at midrapidity (|y|<0.5) by the ALICE Collaboration in proton-proton collisions at a center-of-mass energy √s=13  TeV. They are described within uncertainties by perturbative QCD calculations employing the fragmentation fractions of beauty quarks to baryons measured at forward rapidity by the LHCb Collaboration. The b¯b production cross section per unit of rapidity at midrapidity, estimated from these measurements, is dσb¯b/dy||y|<0.5=83.1±3.5(stat)±5.4(syst)+12.3−3.2(extrap)  μb. The baryon-to-meson ratios are computed to investigate the hadronization mechanism of beauty quarks. The nonprompt Λ+c/D0 production ratio has a similar trend to the one measured for the promptly produced charmed particles and to the p/π+ and Λ/K0S ratios, suggesting a similar baryon-formation mechanism among light, strange, charm, and beauty hadrons. The pT -integrated nonprompt Λ+c/D0 ratio is found to be significantly higher than the one measured in e+e− collisions.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.subject.otherhadron-hadron interactions
dc.subject.otherparticle production
dc.titleStudy of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at √ s = 13 TeV
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202403152466
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2470-0010
dc.relation.numberinseries11
dc.relation.volume108
dc.type.versionpublishedVersion
dc.rights.copyright© 2023 CERN
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber346328
dc.relation.grantnumber346327
dc.subject.ysohiukkasfysiikka
dc.subject.ysohadronit
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p39838
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.108.112003
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundinginformationIn addition, individual groups or members have received support from: European Research Council, Strong 2020—Horizon 2020 (Grant No. 950692, No. 950692), European Union; Academy of Finland (Center of Excellence in Quark Matter) (Grant No. 346327, No. 346328), Finland.
dc.type.okmA1


Aineistoon kuuluvat tiedostot

Thumbnail

Aineisto kuuluu seuraaviin kokoelmiin

Näytä suppeat kuvailutiedot

CC BY 4.0
Ellei muuten mainita, aineiston lisenssi on CC BY 4.0