Non-perturbative heavy quark diffusion coefficients in arbitrarily magnetized quark-gluon plasma
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| Main Authors: | , , , |
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| Format: | Preprint |
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2026
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| _version_ | 1866911626566828032 |
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| author | Dey, Debarshi Bandyopadhyay, Aritra Sun, Yifeng Das, Santosh K. |
| author_facet | Dey, Debarshi Bandyopadhyay, Aritra Sun, Yifeng Das, Santosh K. |
| contents | Heavy quark (HQ) momentum ($κ$) and spatial diffusion ($D_s$) coefficients are computed in a non-perturbative thermal QCD medium in the presence of a background magnetic field of arbitrary strength. Both perturbative and non-perturbative effects are incorporated via the in-medium HQ potential, obtained from the resummed gluon propagator. We find that the momentum diffusion coefficients become anisotropic even in the static heavy quark limit, with the magnetic field direction defining the axis of anisotropy. This anisotropy originates from restrictions on longitudinal momentum diffusion in the gluon spectral function, and naturally leads to two spatial diffusion coefficients ($D_s^L$, $D_s^T$). Non-perturbative effects are found to be dominant at low temperatures. These results provide a more consistent input for Langevin based calculations of the heavy quark directed flow at RHIC and LHC energies. |
| format | Preprint |
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arxiv_https___arxiv_org_abs_2604_24535 |
| institution | arXiv |
| publishDate | 2026 |
| record_format | arxiv |
| spellingShingle | Non-perturbative heavy quark diffusion coefficients in arbitrarily magnetized quark-gluon plasma Dey, Debarshi Bandyopadhyay, Aritra Sun, Yifeng Das, Santosh K. High Energy Physics - Phenomenology Nuclear Theory Heavy quark (HQ) momentum ($κ$) and spatial diffusion ($D_s$) coefficients are computed in a non-perturbative thermal QCD medium in the presence of a background magnetic field of arbitrary strength. Both perturbative and non-perturbative effects are incorporated via the in-medium HQ potential, obtained from the resummed gluon propagator. We find that the momentum diffusion coefficients become anisotropic even in the static heavy quark limit, with the magnetic field direction defining the axis of anisotropy. This anisotropy originates from restrictions on longitudinal momentum diffusion in the gluon spectral function, and naturally leads to two spatial diffusion coefficients ($D_s^L$, $D_s^T$). Non-perturbative effects are found to be dominant at low temperatures. These results provide a more consistent input for Langevin based calculations of the heavy quark directed flow at RHIC and LHC energies. |
| title | Non-perturbative heavy quark diffusion coefficients in arbitrarily magnetized quark-gluon plasma |
| topic | High Energy Physics - Phenomenology Nuclear Theory |
| url | https://arxiv.org/abs/2604.24535 |