2018
No stable wormholes in Einstein-dilaton-Gauss-Bonnet theory
CUYUBAMBA, Marco Antonio, Roman KONOPLYA and Olexandr ZHYDENKOBasic 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.