J 2018

No stable wormholes in Einstein-dilaton-Gauss-Bonnet theory

CUYUBAMBA, Marco Antonio, Roman KONOPLYA and Olexandr ZHYDENKO

Basic information

Original name

No stable wormholes in Einstein-dilaton-Gauss-Bonnet theory

Authors

CUYUBAMBA, Marco Antonio (604 Peru), Roman KONOPLYA (804 Ukraine, guarantor, belonging to the institution) and Olexandr ZHYDENKO (804 Ukraine)

Edition

Physical Review D, 2018, 2470-0010

Other information

Language

English

Type of outcome

Article in a journal

Field of Study

10308 Astronomy

Country of publisher

United States of America

Confidentiality degree

is not subject to a state or trade secret

References:

Impact factor

Impact factor: 4.368

RIV identification code

RIV/47813059:19240/18:A0000253

Organization unit

Faculty of Philosophy and Science in Opava

UT WoS

000442671700006

Keywords in English

Einstein-dilaton-Gauss-Bonnet theory; wormhole; higher-dimensional theory; stability

Tags

International impact, Reviewed
Changed: 4/4/2019 12:21, RNDr. Jan Hladík, Ph.D.

Abstract

V originále

In [Aneesh, S.; Bose, Sukanta; Kar, Sayan : Gravitational waves from quasinormal modes of a class of Lorentzian wormholes. PHYSICAL REVIEW D 97(12):124004] it was shown that the four-dimensional Einstein-dilaton-Gauss-Bonnet theory allows for wormholes without introducing any exotic matter. The numerical solution for the wormhole was obtained there and it was claimed that this solution is gravitationally stable against radial perturbations, what, by now, would mean the only known theoretical possibility for the existence of an apparently stable, four-dimensional and asymptotically flat wormhole without exotic matter. Here, more detailed analysis of perturbations shows that the Kanti-Kleihaus-Kunz wormhole is unstable against small perturbations for any values of its parameters. The exponential growth appears in the time domain after a long period of damped oscillations, in the sameway as it takes place in the case of unstable higher-dimensional black holes in the Einstein-Gauss-Bonnet theory. The instability is driven by the purely imaginary mode, which is nonperturbative in the Gauss-Bonnet coupling alpha.