Skip to content
DraconiticResearch
Search Sources API
203,234 studies31 sourcesUpdated 57 min ago
PreprintarXiv licencearXiv

A unifying zero-mass equation

Abstract

We introduce the nonlocal zero-mass equation − Δu + Φu(|x|) |u|p−2 u = f(u) in ℝN, Φu(r) = a ∫r∞ ρ−b huq−1(ρ) dρ, where hu(ρ) is the mass of |u|p in the ball of radius ρ. For radial functions, this equation includes the defocusing inverse-power Schrödinger equation, the Chern-Simons-Schrödinger equation, and the Schrödinger-Poisson-Slater equation as special cases. We develop the associated ball-mass Lebesgue and Sobolev spaces, which are uniformly convex, and prove sharp compact radial embeddings above a new critical exponent, a Brézis-Lieb type splitting, and a Pohožaev identity. Exploiting a scaling invariance of the operator, we construct an unbounded sequence of eigenvalues of a scaled eigenvalue problem using the Fadell-Rabinowitz cohomological index, and obtain existence and multiplicity results in the subscaled, superscaled, and critical regimes. Our main result is a Brézis-Nirenberg type theorem, proved by means of a new scaled linking theorem, which gives a nontrivial radial solution for every λ> 0 that is not an eigenvalue. Specializing to the three models recovers several known results in a unified way and yields new ones, including a Brézis-Nirenberg type result for the Schrödinger-Poisson-Slater equation in dimensions N ≥ 4.

Related

  1. On the optimal decay rate of global solutions to the convection-diffusion equation with zero-mass initial data
    Yi C. Huang, Ryunosuke Kusaba
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  2. Nodal radial solutions for a zero-mass (p,q)-Laplacian equation with Hardy-Hénon type weight
    José Carlos de Albuquerque, Jonison Carvalho, Eudes Barboza
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  3. Uniqueness of prescribed-node radial bound states for a zero-mass double-power equation
    Wenjing Chen, Zexi Wang
    arXivPreprintCC BY 4.0Full textAnalysis & PDEsarXiv
  4. New sharp lifespan estimates for a semilinear heat equation with zero-mass sign-changing initial data
    Berikbol T. Torebek
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  5. THE ZERO-DISPERSION LIMIT OF THE PERIODIC BENJAMIN-ONO EQUATION FOR SQUARE-INTEGRABLE DATA
    Xi Chen
    HALPreprintCC BY 4.0Full textGeneral mathematicsHAL
BibTeX
@misc{perera2026unifying,
  title = {{A unifying zero-mass equation}},
  author = {Kanishka Perera},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.26585},
  eprint = {2609.26585},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.26585},
}
RIS
TY  - UNPB
TI  - A unifying zero-mass equation
AU  - Kanishka Perera
PY  - 2026
DA  - 2026/09/22
PB  - arXiv
DO  - 10.48550/arxiv.2609.26585
UR  - https://arxiv.org/abs/2609.26585
AB  - We introduce the nonlocal zero-mass equation − Δu + Φ_u(|x|) |u|^p−2 u = f(u) in ℝ^N, Φ_u(r) = a ∫_r^∞ ρ^−b h_u^q−1(ρ) dρ, where h_u(ρ) is the mass of |u|^p in the ball of radius ρ. For radial functions, this equation includes the defocusing inverse-power Schrödinger equation, the Chern-Simons-Schrödinger equation, and the Schrödinger-Poisson-Slater equation as special cases. We develop the associated ball-mass Lebesgue and Sobolev spaces, which are uniformly convex, and prove sharp compact radial embeddings above a new critical exponent, a Brézis-Lieb type splitting, and a Pohožaev identity. Exploiting a scaling invariance of the operator, we construct an unbounded sequence of eigenvalues of a scaled eigenvalue problem using the Fadell-Rabinowitz cohomological index, and obtain existence and multiplicity results in the subscaled, superscaled, and critical regimes. Our main result is a Brézis-Nirenberg type theorem, proved by means of a new scaled linking theorem, which gives a nontrivial radial solution for every λ> 0 that is not an eigenvalue. Specializing to the three models recovers several known results in a unified way and yields new ones, including a Brézis-Nirenberg type result for the Schrödinger-Poisson-Slater equation in dimensions N ≥ 4.
ER  -