2019
DOI: 10.1016/j.physletb.2019.01.046
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Quasinormal modes of scalarized black holes in the Einstein–Maxwell–Scalar theory

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Cited by 92 publications
(62 citation statements)
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“…Here the instability arises when the product −β 0 T , where β 0 is the effective linear matter-scalar coupling and T is the trace of the stress-energy tensor, is larger than some critical value [33]: spontaneous scalarization in neutron stars is induced by couplings with matter (see also [34,35]). Later it was realized that spontaneous scalarization can occur for charged black holes in Einstein-Maxwell-scalar (EMs) theory, for certain choices of the scalar coupling function and coupling strength [36][37][38][39][40][41]. This "charge-induced" spontaneous scalarization presents many similarities with the case of curvature-induced spontaneous scalarization of black holes [24][25][26][27][28][29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…Here the instability arises when the product −β 0 T , where β 0 is the effective linear matter-scalar coupling and T is the trace of the stress-energy tensor, is larger than some critical value [33]: spontaneous scalarization in neutron stars is induced by couplings with matter (see also [34,35]). Later it was realized that spontaneous scalarization can occur for charged black holes in Einstein-Maxwell-scalar (EMs) theory, for certain choices of the scalar coupling function and coupling strength [36][37][38][39][40][41]. This "charge-induced" spontaneous scalarization presents many similarities with the case of curvature-induced spontaneous scalarization of black holes [24][25][26][27][28][29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%
“…Regularity of the scalar field at the origin then requires the coupling to diverge as ∼ 1/r 2N +2 . From (12) this implies that the energy density is finite therein and from (6),…”
Section: Everywhere Regular Solutionsmentioning
confidence: 97%
“…This means that even though the electrovacuum Reissner-Nordström (RN) black hole is a solution of the EMS model, for sufficiently high charge to mass ratio this black hole becomes unstable: it becomes energetically favourable for the RN black hole to scalarise. A new family of scalarised black holes bifurcates from the RN family, which contains the end states of this dynamical scalarisation mechanism -see also [9][10][11][12][13][14][15].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, a novel approach to trigger black hole scalar hairs was provided by considering non-minimal couplings between scalar fields and the Gauss-Bonnet invariant [49][50][51][52][53][54][55]. Moreover, it was found that this scalar-Gauss-Bonnet coupling can lead to scalar condensations in various black hole models [56][57][58][59][60][61][62][63][64]. Inspired by these black hole properties, in the background of neutral reflecting compact stars, we have constructed scalar hairy configurations by including scalar-Gauss-Bonnet couplings with numerical methods [65].…”
Section: Introductionmentioning
confidence: 99%