Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 7 min ago
PreprintCC0arXiv

Navier-Stokes hydrodynamics near the critical point with out-of-equilibrium modes

Abstract

We investigate how slow out-of-equilibrium modes (OEM), introduced to extend the regime of validity of hydrodynamics near the critical point, fundamentally reshape the power spectrum of dynamical density fluctuations. We have used the equation of motion of slow modes for the situation when the extensive nature of thermodynamics is not altered due to the introduction of OEM. We find that the extensivity condition puts an extra constraint on the coupling of OEM with the four divergence of velocity. In the absence of OEM, the dynamic structure factor exhibits three Lorentzian peaks, one at zero frequency (ω), called Rayleigh peak and the other two called Brillouin peaks located symmetrically about ω=0. When the system is away from the critical point the inclusion of the OEM preserves the symmetry of the distributions but all the peaks acquire reduced widths and the Brillouin peaks adopt unequal heights. Irrespective of the value of OEM (zero or nonzero) the Brillouin peaks vanish near the critical point. The width of the Rayleigh peak substantially reduced in presence of OEM. Such reductions of the widths in presence of the OEM indicates the reduction in the decay rate of the fluctuation which leads to slowing down of decay of the fluctuations, a distinctive feature of the critical point.

Related

  1. Searching for the QCD critical point with relativistic viscous hydrodynamics
    Kevin P. Pala, Surkhab K. Virk, Isabella Danhoni +3
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsNuclear physicsarXiv
  2. Solving the Incompressible Navier-Stokes Equations on Oriented Curved Surfaces Discretized by Point Clouds
    Alejandra Foggia, Ivo F. Sbalzarini
    arXivPreprintCC BY 4.0Full textNumerical analysis & scientific computingComputational physicsarXiv
  3. Exploring Dynamical Quantum Phase Transitions via the Dynamical Phase Accumulated at an Equilibrium Critical Point
    Han-Chuan Kou, Peng Li, Zhi-Han Zhang +1
    arXivPreprintCC BY 4.0Full textQuantum physics & quantum informationarXiv
  4. The Navier-Stokes equations blow up, and planes still fly
    Amin Doostmohammadi
    Communications PhysicsPeer-reviewedCC BY-NC-ND 4.0Full textAtomic, molecular & optical physicsCrossref
  5. High-order immersed boundary method for subsonic aeroacoustics and compressible Navier-Stokes equationsHigh-order immersed boundary method for subsonic aeroacoustics and compressible Navier-Stokes equations
    Abdoulaye Ouattara, David Marx, Christian Prax +3
    arXivPreprintCC BY-NC-ND 4.0Full textFluid dynamicsarXiv
BibTeX
@misc{hasanujjaman2026navierstokes,
  title = {{Navier-Stokes hydrodynamics near the critical point with out-of-equilibrium modes}},
  author = {Md Hasanujjaman and Golam Sarwar and Mahfuzur Rahaman and Abhijit Bhattacharyya and Jane Alam},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.24844},
  eprint = {2609.24844},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.24844},
  note = {CC0},
}
RIS
TY  - UNPB
TI  - Navier-Stokes hydrodynamics near the critical point with out-of-equilibrium modes
AU  - Md Hasanujjaman
AU  - Golam Sarwar
AU  - Mahfuzur Rahaman
AU  - Abhijit Bhattacharyya
AU  - Jane Alam
PY  - 2026
DA  - 2026/09/21
PB  - arXiv
DO  - 10.48550/arxiv.2609.24844
UR  - https://arxiv.org/abs/2609.24844
AB  - We investigate how slow out-of-equilibrium modes (OEM), introduced to extend the regime of validity of hydrodynamics near the critical point, fundamentally reshape the power spectrum of dynamical density fluctuations. We have used the equation of motion of slow modes for the situation when the extensive nature of thermodynamics is not altered due to the introduction of OEM. We find that the extensivity condition puts an extra constraint on the coupling of OEM with the four divergence of velocity. In the absence of OEM, the dynamic structure factor exhibits three Lorentzian peaks, one at zero frequency (ω), called Rayleigh peak and the other two called Brillouin peaks located symmetrically about ω=0. When the system is away from the critical point the inclusion of the OEM preserves the symmetry of the distributions but all the peaks acquire reduced widths and the Brillouin peaks adopt unequal heights. Irrespective of the value of OEM (zero or nonzero) the Brillouin peaks vanish near the critical point. The width of the Rayleigh peak substantially reduced in presence of OEM. Such reductions of the widths in presence of the OEM indicates the reduction in the decay rate of the fluctuation which leads to slowing down of decay of the fluctuations, a distinctive feature of the critical point.
ER  -