Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/13317
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dc.contributor.authorDey, Jayantaen_US
dc.date.accessioned2024-03-19T12:57:03Z-
dc.date.available2024-03-19T12:57:03Z-
dc.date.issued2024-
dc.identifier.citationSatapathy, S., De, S., Dey, J., & Ghosh, S. (2024). Spatial diffusion of heavy quarks in a background magnetic field. Physical Review C. Scopus. https://doi.org/10.1103/PhysRevC.109.024904en_US
dc.identifier.isbn000-0000000000-
dc.identifier.issn2469-9985-
dc.identifier.otherEID(2-s2.0-85184823864)-
dc.identifier.urihttps://doi.org/10.1103/PhysRevC.109.024904-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/13317-
dc.description.abstractThe ratio of shear viscosity to entropy density shows a valley-shaped pattern well-known in the community of heavy-ion physics. Diffusion coefficients of heavy quark and meson show a similar structure, and both sketches have become quite popular in the community. Present work has attempted a finite magnetic field extension of the diffusion coefficients of heavy quark and meson. Using Einstein's diffusion relation, we calculated heavy quark and heavy meson diffusion by the ratio of conductivity to susceptibility in the kinetic theory framework of relaxation time approximation. The relaxation time of heavy quark and meson are tuned from the knowledge of earlier works on spatial diffusion estimations, and then we have extended the framework for a finite magnetic field, where our outcomes have revealed two aspects - anisotropic and quantum aspects of diffusion with future possibilities of phenomenological signature. © 2024 authors. Published by the American Physical Society.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.sourcePhysical Review Cen_US
dc.titleSpatial diffusion of heavy quarks in a background magnetic fielden_US
dc.typeJournal Articleen_US
dc.rights.licenseAll Open Access, Hybrid Gold, Green-
Appears in Collections:Department of Physics

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