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− (−K2 +zK 3)G(c, z,2,1) z2((−1 +z 2)K 2 2 + 5zK2K3 −z 2K 2 3))−1,(C1) A12 = ˆγ((K2 −zK 3)G(c, z,1,1)/K 2 −G(c, z,2,1) z2 p ((−1 +z 2)K 2 2 + 5zK2K3 −z 2K 2 3) ),(C2) A13 = ˆγ z2 (

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hep-ph 1

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2025 1

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Normal mode analysis within relativistic massive transport

hep-ph · 2025-05-07 · unverdicted · novelty 7.0

Normal mode analysis of the relativistic Boltzmann equation for massive particles reveals coupling between sound and heat channels, mass-dependent critical wavenumbers, and an infinite branch cut for Landau damping.

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  • Normal mode analysis within relativistic massive transport hep-ph · 2025-05-07 · unverdicted · none · ref 5

    Normal mode analysis of the relativistic Boltzmann equation for massive particles reveals coupling between sound and heat channels, mass-dependent critical wavenumbers, and an infinite branch cut for Landau damping.