Abstract

We study geodesic motion near the throats of asymptotically flat, static, spherically symmetric traversable wormholes supported by a self-gravitating minimally coupled phantom scalar field with an arbitrary self-interaction potential. We assume that any such wormhole possesses the reflection symmetry with respect to the throat, and consider only its observable “right half”. It turns out that the main features of bound orbits and photon trajectories close to the throats of such wormholes are very different from those near the horizons of black holes. We distinguish between wormholes of two types, the first and second ones, depending on whether the redshift metric function has a minimum or maximum at the throat. First, it turns out that orbits located near the centre of a wormhole of any type exhibit retrograde precession, that is, the angle of pericentre precession is negative. Second, in the case of high accretion activity, wormholes of the first type have the innermost stable circular orbit at the throat while those of the second type have the resting-state stable circular orbit in which test particles are at rest at all times. In our study, we have in mind the possibility that the strongly gravitating objects in the centres of galaxies are wormholes, which can be regarded as an alternative to black holes, and the scalar field can be regarded as a realistic model of dark matter surrounding galactic centres. In this connection, we discuss qualitatively some observational aspects of results obtained in this article.

Highlights

  • The centres of galaxies are usually recognized to be supermassive black holes [1,2,3], but we still do not have a completely reliable identification of these objects [4,5]

  • We have examined two types of scalar field wormholes and found some distinctive features of timelike bound orbits located in the vicinities of the wormhole throats, and of the trajectories of null geodesics

  • A scalar field models dark matter surrounding the centres of normal galaxies

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Summary

Introduction

The centres of galaxies are usually recognized to be supermassive black holes [1,2,3], but we still do not have a completely reliable identification of these objects [4,5]. Universe 2020, 6, 183 approach, in which dark matter is modelled by a scalar field [24,25] while effects of rotation are not taken into account; the problem can be analytically tractable This approach allows us to explore some unevident features of the trajectories of massive and massless test particles in such spacetimes; these features are usually hidden in qualitative models based on computer simulations. Distinctive features of geodesic motion near the throat of a phantom scalar field wormhole can be used to identify observationally the central objects in galaxies, and to test general relativity in a strong gravitational regime in order to distinguish between some dark matter models and the hypothetical fifth force [35].

Scalar Field Wormholes
Timelike and Null Geodesics
Timelike Geodesics
Null Geodesics
Two Examples of Wormholes
Trajectories of Timelike Geodesics
Trajectories of Null Geodesics
Discussion
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