Exact Static Solutions for Scalar Fields Coupled to Gravity in $(3+1)$-Dimensions

Abstract

Einstein&#39;s field equations for a spherically symmetric metric coupled to a massless scalar field are reduced to a system effectively of second order in time, in terms of the variables $μ=m/r$ and $y=(α/ra)$, where $a$, $α$, $r$ and $m$ are as in [W.M. Choptuik, ``Universality and Scaling in Gravitational Collapse of Massless Scalar Field&#34;, \textit{Physical Review Letters} {\bf{70}} (1993), 9-12]. Solutions for which $μ$ and $y$ are time independent may arise either from scalar fields with $ϕ_t=0$ or with $ϕ_s=0$ but $ϕ$ linear in $t$, called respectively the positive and negative branches having the Schwarzschild solution characterized by $ϕ=0 $ and $μ_s+μ=0$ in common. For the positive branch we obtain an exact solution which have been in fact obtained first in [I.Z. Fisher,``Scalar mesostatic field with regard for gravitational effects&#34;, \textit{Zh. Eksp. Teor. Fiz.} {\bf{18}} (1948), 636-640, gr-qc/9911008] and rediscovered many times (see D. Grumiller, ``Quantum dilaton gravity in two dimensions with matter&#34;, PhD thesis, \textit{Technische Universit$\ddot{a}$t, Wien} (2001), gr-qc/0105078) and we prove that the trivial solution $μ=0$ is a global attractor for the region $μ_s+μ>0 $, $μ<1/2$. For the negative branch discussed first in [M. Wyman, ``Static spherically symmetric scalar fields in general relativity&#34;, \textit{Physical Review D} {\bf{24}} (1981), 839-841] perturbatively, we prove that $μ=0$ is a saddle point for the linearized system, but the non-vacuum solution $μ=1/4$ is a stable focus and a global attractor for the region $μ_s+μ>0$, $μ<1/2$.