The Lifetime of Axion Stars

Joshua Eby; Peter Suranyi; L. C. R. Wijewardhana

doi:10.1142/S0217732316500905

paper

The Lifetime of Axion Stars

arXiv:1512.01709 · doi:10.1142/S0217732316500905

Abstract

We investigate the decay of condensates of scalars in a field theory defined by $V (A) = m^{2} f^{2} [1 - cos (A / f)]$ , where $m$ and $f$ are the mass and decay constant of the scalar field. An example of such a theory is that of the axion, in which case the condensates are called axion stars. The axion field, $A$ , is self adjoint. As a result the axion number is not an absolutely conserved quantity. Therefore, axion stars are not stable and have finite lifetimes. Bound axions, localized on the volume of the star, have a coordinate uncertainty $Δ x \sim R \sim 1/ (m_{a} Δ)$ , where $R$ is the radius of the star and $Δ = 1 - E_{0}^{2} / m_{a}^{2}$ . Here $m_{a}$ and $E_{0}$ are the mass, and the ground state energy of the bound axion. Then the momentum distribution of axions has a width of $Δ p \sim m_{a} Δ$ . At strong binding, $Δ = O (1)$ , bound axions can easily transfer a sufficient amount of momentum to create and emit a free axion, leading to fast decay of the star with a transition rate $Γ \sim m_{a}$ . However, when $Δ ≪ 1$ , the momentum distribution is more restricted, and as shown in this paper, the transition rate for creating a free axion decreases as $exp (- p Δ x) \sim exp (- Δ^{- 1})$ . Then sufficiently large, weakly bound axion stars, produced after the big bang, survive until the present time. We plot the region of their stability, limited by decay through axion loss and by gravitational instability, as a function of the mass of the axion and the mass of the star.

19 pages, 3 figures. v2: typos corrected, 1 figure corrected, 1 figure added. v3: typos corrected

The Lifetime of Axion Stars

Abstract

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