2020
DOI: 10.1103/physrevd.102.024050
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Onset of spontaneous scalarization in generalized scalar-tensor theories

Abstract: In gravity theories that exhibit spontaneous scalarization, astrophysical objects are identical to their general relativistic counterpart until they reach a certain threshold in compactness or curvature. Beyond this threshold, they acquire a non-trivial scalar configuration, which also affects their structure. The onset of scalarization is controlled only by terms that contribute to linear perturbation around solutions of general relativity. The complete set of these terms has been identified for generalized s… Show more

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Cited by 41 publications
(37 citation statements)
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“…Compact stars can scalarize for η < 0 [33] and hence yield constraints. However, this effect could easily be quenched by adding a coupling between the scalar field and the Ricci scalar [41,60]. The latter might be necessary to get a sensible cosmology [61], and would have no effect for black holes, thus leaving our analysis unaffected.…”
Section: Resultsmentioning
confidence: 99%
“…Compact stars can scalarize for η < 0 [33] and hence yield constraints. However, this effect could easily be quenched by adding a coupling between the scalar field and the Ricci scalar [41,60]. The latter might be necessary to get a sensible cosmology [61], and would have no effect for black holes, thus leaving our analysis unaffected.…”
Section: Resultsmentioning
confidence: 99%
“…The fact that the onset of scalarization is captured in linear theory allows one to identify all possible couplings to curvature that can lead to scalarization [31] and simplifies the investigation of the relevant thresholds [32]. It also makes it straightforward to generalize the mechanism to nongravitational couplings (see, e.g., [33,34]).…”
mentioning
confidence: 99%
“…Originally, spontaneous scalarization has been identified for spherically symmetric NS models in a class of massless ST theories sometimes refered to as Bergmann-Wagoner [22,23] theories; these complement the metric sector of GR with a single scalar field, are governed by second-order covariant field Equations at most linear in second and quadratic in first derivatives, and obey the weak equivalence principle. The phenomenon has by now been demonstrated to occur over a wide range of configurations and also in other theoretical frameworks [24,25]. Analogous phenomena occur in many scenarios involving fields non-minimally coupled to a spacetime metric.…”
Section: Introductionmentioning
confidence: 72%