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Effects of Schwarzschild's Black Hole Singularities on Complex Scalar Field

Z. E. Musielak, J. L. Fry, G. W. Kanan

Abstract

Complex scalar fields described by a novel Klein-Gordon equation derived from gauge and group theories are considered at the Schwarzschild's black hole singularities. It is shown that the field is well-behaved in the vicinity of these singularities and that its value reaches zero at both singularities. The obtained results also demonstrate that the field forms a scalar hair that exists outside of the event horizon, and that the interior field is tachyonic and undergoes a tachyonic condensation to reach its true vacuum at the central singularity. The described field's behavior is very different from that predicted by the Klein-Gordon equation minimally coupled to gravity. Physical implications of these results for the interior structure of black holes are discussed.

Effects of Schwarzschild's Black Hole Singularities on Complex Scalar Field

Abstract

Complex scalar fields described by a novel Klein-Gordon equation derived from gauge and group theories are considered at the Schwarzschild's black hole singularities. It is shown that the field is well-behaved in the vicinity of these singularities and that its value reaches zero at both singularities. The obtained results also demonstrate that the field forms a scalar hair that exists outside of the event horizon, and that the interior field is tachyonic and undergoes a tachyonic condensation to reach its true vacuum at the central singularity. The described field's behavior is very different from that predicted by the Klein-Gordon equation minimally coupled to gravity. Physical implications of these results for the interior structure of black holes are discussed.

Paper Structure

This paper contains 20 sections, 36 equations, 2 figures.

Figures (2)

  • Figure 1: The normalized potential $V (r_o, \Phi) / \Omega^2$ is plotted as a function of the outside field $\Phi$ for several fixed values of $r_o > R_S$.
  • Figure 2: The normalized potential $V (r, \Phi) / \Omega^2$ is plotted as a function of the inside field $\Phi$ for several fixed values of $r > R_S$.