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March 2, 2026Calculus of Variations and Partial Differential Equations0 citationsOpen Access

Normalised solutions and limit profiles of the defocusing Gross–Pitaevskii–Poisson equation

RMRiccardo MolleVMVitaly MorozGRGiuseppe Riey

Key Points

  • To investigate the existence of normalised solutions for the stationary Gross–Pitaevskii–Poisson equation and their characteristics.
  • Analysis of normalised solutions of the GPP equation with a defocusing nonlinear term.
  • Mathematical exploration of mass-energy relation curves.
  • Examination of limit profiles at endpoints of these curves.
  • Establishment of branches of normalised solutions for the GPP equation.
  • Identification of significant variations in the behaviour of solutions based on different parameters.
  • Insights into the implications of normalised solutions for models of self-gravitating systems.

Abstract

Abstract We consider normalised solutions of the stationary Gross–Pitaevskii–Poisson (GPP) equation with a defocusing local nonlinear term, aligned - u+ u+|u|²u = (I_ *|u|²) u in R³, ₑ³u²dx= ², aligned - Δ u + λ u + | u | 2 u = (I α ∗ | u | 2) u in R 3, ∫ R 3 u 2 d x = ρ 2, where ²>0 ρ 2 > 0 is the prescribed mass of the solutions, R λ ∈ R is an a-priori unknown Lagrange multiplier, and I_ (x) =A_ |x|^3- I α (x) = A α | x | 3 - α is the Riesz potential of order (0, 3) α ∈ (0, 3). When =2 α = 2 this problem appears in the models of self–gravitating Bose–Einstein condensates, which were proposed in cosmology and astrophysics to describe Cold Dark Matter and Boson Stars. We establish the existence of branches of normalised solutions to the GPP equation, paying special attention to the shape of the associated mass–energy relation curves and to the limit profiles of solutions at the endpoints of these curves. The behaviour of normalised solutions depends sensitively on whether

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Cite This Study

Molle et al. (2026) studied this question.

synapsesocial.com/papers/69a52de5f1e85e5c73bf1067https://doi.org/10.1007/s00526-026-03268-7
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