Onset of rotating scalarized black holes in Einstein-Chern-Simons-Scalar theory
We perform the stability analysis of the Kerr black hole in the Einstein-Chern-Simons-Scalar theory with quadratic scalar coupling. For positive coupling parameter (α>0), we introduce the (2+1)-dimensional hyperboloidal foliation method to show that the Kerr black hole is unstable against scalar-...
Saved in:
Published in | Physics letters. B Vol. 814; p. 136081 |
---|---|
Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
10.03.2021
Elsevier |
Online Access | Get full text |
Cover
Loading…
Summary: | We perform the stability analysis of the Kerr black hole in the Einstein-Chern-Simons-Scalar theory with quadratic scalar coupling. For positive coupling parameter (α>0), we introduce the (2+1)-dimensional hyperboloidal foliation method to show that the Kerr black hole is unstable against scalar-mode perturbation. In case of α<0, it is shown that the Kerr black hole is unstable without any α-independent bound on the rotation parameter a when using the hyperboloidal foliation method. The disappearance of the a-bound is confirmed analytically by implementing the (1+1)-dimensional linearized scalar equation. |
---|---|
ISSN: | 0370-2693 1873-2445 |
DOI: | 10.1016/j.physletb.2021.136081 |