Pith. sign in

REVIEW 1 cited by

Damping versus oscillations for a gravitational Vlasov-Poisson system

Not yet reviewed by Pith; the record is open.

This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.

SPECIMEN: schema-true, not a live event

T0 review · schema-true

One-sentence machine reading of the paper's core claim.

pith:XXXXXXXX · record.json · timestamp

arxiv 2301.07662 v1 pith:KJLBEC2I submitted 2023-01-18 math.AP math-phmath.MP

classification math.APmath-phmath.MP
keywords gravitationalsteadysystemvlasov-poissonboundarydichotomyperturbationsproof
verification ladder T0 review T1 audit T2 compute T3 formal
0 comments
abstract

We consider a family of isolated inhomogeneous steady states to the gravitational Vlasov-Poisson system with a point mass at the centre. They are parametrised by the polytropic index $k>1/2$, so that the phase space density of the steady state is $C^1$ at the vacuum boundary if and only if $k>1$. We prove the following sharp dichotomy result: if $k>1$ the linear perturbations Landau damp and if $1/2< k\le1$ they do not. The above dichotomy is a new phenomenon and highlights the importance of steady state regularity at the vacuum boundary in the discussion of long-time behaviour of the perturbations. Our proof of (nonquantitative) gravitational relaxation around steady states with $k>1$ is the first such result for the gravitational Vlasov-Poisson system. The key step in the proof is to show that no embedded eigenvalues exist in the essential spectrum of the linearised system.

Discussion (0). Continue with ORCID to comment.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. On quantitative linear gravitational relaxation

    math.AP 2025-05 conditional novelty 8.0 of 10

    For small polytropic galaxies with a central point mass, the gravitational force from linear perturbations decays as (1+t)^{-b}, with decay order set by initial-data and steady-state regularity.

Pith tools