Phonon number relaxation in a 3D superfluid with a concave acoustic branch.
Abstract
We consider the collisional evolution towards equilibrium of a spatially homogeneous and isotropic phonon gas of a three-dimensional superfluid with a concave acoustic excitation branch, at a non-zero but arbitrarily low temperature T. Three-phonon collisions 1ϕ↔ 2ϕ are forbidden by conservation of energy-momentum. Four-phonon collisions 2ϕ→ 2ϕ of Landau and Khalatnikov lead, after a time ∝ T−7, only to a partial thermal equilibrium, a Bose law of non-zero chemical potential for the phonons, because they conserve the total number of phonons. Relaxation towards complete thermochemical equilibrium is therefore ensured by the much slower five-phonon collisions 2ϕ↔ 3ϕ of Khalatnikov, in a time ∝ T−9. Using kinetic equations on the occupation numbers of the phonon modes and explicitly calculating the 2ϕ→ 3ϕ collisional amplitude with quantum hydrodynamics at low temperature, we determine the corresponding evolution of the fugacity zϕ of the phonon gas from the non-degenerate regime zϕ=0+ to complete equilibrium zϕ=1-. Using the conservation of total energy, we find that the fugacity varies with a non-integer power law ∝ t4/5 at short times and an exponential law at long times; the speed of change of entropy, always positive, is asymptotically proportional to the square of the speed of change of fugacity, (d/dt)Sϕ∝[(d/dt)zϕ]2, as Landau predicted for an arbitrarily slow adiabatic transformation. Our results bring to a close the study initiated by Khalatnikov in 1950 and could be experimentally verified in a gas of cold spin-1/2 fermionic atoms in the sector of the BEC-BCS crossover where the acoustic branch has a concave start, or in superfluid liquid helium-4 at sufficiently high pressure.
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BibTeX
@article{castin2026phonon,
title = {{Phonon number relaxation in a 3D superfluid with a concave acoustic branch.}},
author = {Yvan Castin and Mariia Tsimokha},
journal = {Comptes Rendus. Physique},
year = {2026},
month = oct,
doi = {10.5802/crphys.292},
eprint = {2604.18298},
archivePrefix = {arXiv},
url = {https://hal.science/hal-05595595v2},
note = {CC BY-NC-ND 4.0},
}
RIS
TY - JOUR
TI - Phonon number relaxation in a 3D superfluid with a concave acoustic branch.
AU - Yvan Castin
AU - Mariia Tsimokha
PY - 2026
DA - 2026/10/14
JO - Comptes Rendus. Physique
DO - 10.5802/crphys.292
UR - https://hal.science/hal-05595595v2
AB - We consider the collisional evolution towards equilibrium of a spatially homogeneous and isotropic phonon gas of a three-dimensional superfluid with a concave acoustic excitation branch, at a non-zero but arbitrarily low temperature T. Three-phonon collisions 1ϕ↔ 2ϕ are forbidden by conservation of energy-momentum. Four-phonon collisions 2ϕ→ 2ϕ of Landau and Khalatnikov lead, after a time ∝ T^−7, only to a partial thermal equilibrium, a Bose law of non-zero chemical potential for the phonons, because they conserve the total number of phonons. Relaxation towards complete thermochemical equilibrium is therefore ensured by the much slower five-phonon collisions 2ϕ↔ 3ϕ of Khalatnikov, in a time ∝ T^−9. Using kinetic equations on the occupation numbers of the phonon modes and explicitly calculating the 2ϕ→ 3ϕ collisional amplitude with quantum hydrodynamics at low temperature, we determine the corresponding evolution of the fugacity z_ϕ of the phonon gas from the non-degenerate regime z_ϕ=0^+ to complete equilibrium z_ϕ=1^-. Using the conservation of total energy, we find that the fugacity varies with a non-integer power law ∝ t^4/5 at short times and an exponential law at long times; the speed of change of entropy, always positive, is asymptotically proportional to the square of the speed of change of fugacity, (d/dt)S_ϕ∝[(d/dt)z_ϕ]^2, as Landau predicted for an arbitrarily slow adiabatic transformation. Our results bring to a close the study initiated by Khalatnikov in 1950 and could be experimentally verified in a gas of cold spin-1/2 fermionic atoms in the sector of the BEC-BCS crossover where the acoustic branch has a concave start, or in superfluid liquid helium-4 at sufficiently high pressure.
SN - 1631-0705
SN - 1878-1535
ER -