Mass-radius relation of Newtonian self-gravitating Bose-Einstein condensates with short-range interactions. I. Analytical results

Pierre-Henri Chavanis

Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology · 2011 · 515 citations · 134 references

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TL;DR

These equations model astrophysical objects such as boson stars and, presumably, dark matter galactic halos, linking the non‑interacting case of Ruffini and Bonazzola (1969) to the Thomas‑Fermi limit of Böhmer and Harko (2007). The study aims to derive an approximate analytical mass‑radius relation for a Newtonian self‑gravitating Bose‑Einstein condensate with short‑range interactions and to examine the radius–scattering‑length dependence at fixed mass. Using the Gross‑Pitaevskii‑Poisson system and a Gaussian ansatz, the authors obtain a tractable analytical expression for the mass‑radius relation and analyze the radius–scattering‑length behavior for a given mass. The analytical solution reveals that repulsive short‑range interactions allow arbitrarily massive configurations with a minimum radius, while attractive interactions permit equilibrium only below a maximum mass, above which collapse to a black hole is expected; equilibrium also requires a scattering length above a negative threshold, and the Gaussian‑ansatz expression agrees with numerical solutions, enabling stability analysis and pulsation‑period estimates via a mechanical analogy.

Abstract

We provide an approximate analytical expression of the mass-radius relation of a Newtonian self-gravitating Bose-Einstein condensate (BEC) with short-range interactions described by the Gross-Pitaevskii-Poisson system. These equations model astrophysical objects such as boson stars and, presumably, dark matter galactic halos. Our study connects the noninteracting case studied by Ruffini and Bonazzola (1969) to the Thomas-Fermi limit studied by B\"ohmer and Harko (2007). For repulsive short-range interactions (positive scattering lengths), there exists configurations of arbitrary mass but their radius is always larger than a minimum value. For attractive short-range interactions (negative scattering lengths), equilibrium configurations only exist below a maximum mass. Above that mass, the system is expected to collapse and form a black hole. We also study the radius versus scattering length relation for a given mass. We find that equilibrium configurations only exist above a (negative) minimum scattering length. Our approximate analytical solution, based on a Gaussian ansatz, provides a very good agreement with the exact solution obtained by numerically solving a nonlinear differential equation representing hydrostatic equilibrium. Our analytical treatment is, however, easier to handle and permits one to study the stability problem, and derive an expression of the pulsation period, by developing an analogy with a simple mechanical problem.

References

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