pith. sign in

Based on the above analysis, the number of obtained modes matches the number of zeros derived from the argument principle

Additionally, we find that in this case z≪1, the sound, heat channels in Φ 1 decouple, resulting in Φ1 (ˆγ, c) = ˆγcoth−1 c−1 3ˆγ(c−ˆγ) + (3cˆγ(ˆγ−c)−ˆγ) coth−1 c+ 1 = 0,(50) as

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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 4

    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.