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dc.contributor.authorBoguslavski, K.
dc.contributor.authorKurkela, A.
dc.contributor.authorLappi, T.
dc.contributor.authorLindenbauer, F.
dc.contributor.authorPeuron, J.
dc.date.accessioned2024-05-03T06:48:28Z
dc.date.available2024-05-03T06:48:28Z
dc.date.issued2024
dc.identifier.citationBoguslavski, K., Kurkela, A., Lappi, T., Lindenbauer, F., & Peuron, J. (2024). Heavy quark diffusion coefficient in heavy-ion collisions via kinetic theory. <i>Physical Review D</i>, <i>109</i>(1), Article 014025. <a href="https://doi.org/10.1103/PhysRevD.109.014025" target="_blank">https://doi.org/10.1103/PhysRevD.109.014025</a>
dc.identifier.otherCONVID_213468966
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/94661
dc.description.abstractWe compute the heavy quark momentum diffusion coefficient κ using QCD kinetic theory for a system going through bottom-up isotropization in the initial stages of a heavy ion collision. We find that the values of κ are within 30% from a thermal system at the same energy density. When matching for other quantities we observe considerably larger deviations. We also observe that the diffusion coefficient in the transverse direction is larger at high occupation numbers, whereas for an underoccupied system the longitudinal diffusion coefficient dominates. The behavior of the diffusion coefficient can be understood on a qualitative level based on the Debye mass mD and the effective temperature of soft modes T∗. Our results for the kinetic evolution of κ in different directions can be used in phenomenological descriptions of heavy quark diffusion and quarkonium dynamics to include the impact of pre-equilibrium stages.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review D
dc.rightsCC BY 4.0
dc.titleHeavy quark diffusion coefficient in heavy-ion collisions via kinetic theory
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202405033287
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.numberinseries1
dc.relation.volume109
dc.type.versionpublishedVersion
dc.rights.copyright© Authors 2024
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber824093
dc.relation.grantnumber824093
dc.relation.grantnumber346324
dc.relation.grantnumber321840
dc.relation.grantnumber835105
dc.relation.grantnumber835105
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/835105/EU//YoctoLHC
dc.subject.ysohiukkasfysiikka
dc.subject.ysokvarkit
dc.subject.ysokvanttiväridynamiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p19627
jyx.subject.urihttp://www.yso.fi/onto/yso/p39318
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevD.109.014025
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramRIA Research and Innovation Action, H2020en
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramERC Advanced Granten
jyx.fundingprogramRIA Research and Innovation Action, H2020fi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundingprogramERC Advanced Grantfi
jyx.fundinginformationThis work is supported by the European Research Council, ERC-2018-ADG-835105 YoctoLHC. This work was also supported under the European Union’s Horizon 2020 research and innovation by the STRONG-2020 project (Grant Agreement No. 824093). The content of this article does not reflect the official opinion of the European Union and responsibility for the information and views expressed therein lies entirely with the authors. This work was funded in part by the Knut and Alice Wallenberg foundation, Contract No. 2017.0036. T. L. and J. P. have been supported by the Academy of Finland, by the Centre of Excellence in Quark Matter (Project No. 346324) and Project No. 321840. K. B. and F. L. would like to thank the Austrian Science Fund (FWF) for support under Project No. P 34455, and F. L. is additionally supported by the Doctoral Program W1252-N27 Particles and Interactions. The authors wish to acknowledge CSC–IT Center for Science, Finland, for computational resources. We acknowledge grants of computer capacity from the Finnish Grid and Cloud Infrastructure (persistent identifier urn:nbn:fi:research-infras-2016072533). The authors also wish to acknowledge the Vienna Scientific Cluster (VSC) project 71444 for computational resources.
dc.type.okmA1


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