4.7 Article

Spin-induced dynamical scalarization, descalarization, and stealthness in scalar-Gauss-Bonnet gravity during a black hole coalescence

Journal

PHYSICAL REVIEW D
Volume 106, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.106.044018

Keywords

-

Funding

  1. NSF
  2. Royal Society (UK) Research [OAC-2004879, PHY-2110416, RGF\R1\180073, 896696, TG-PHY210114]
  3. Simons Foundation [ACI-1548562]
  4. Science and Technology Facilities Council (STFC) [OCI-0725070]
  5. Extreme Science and Engineering Discovery Environment (XSEDE) Expanse through the allocation
  6. State of Illinois and the National Geospatial Intelligence Agency (Blue Waters is a joint effort of the University of Illinois at Urbana-Champaign and its National Center for Supercomputing Applications) [ACI-1238993]
  7. University of Illinois at Urbana-Champaign
  8. MINERVA cluster at the Max Planck Institute for Gravitational Physics
  9. Leibnitz Supercomputing Centre SuperMUC-NG
  10. Juelich Supercomputing Center JUWELS HPC [2018194669]
  11. COSMA7 in Durham and Leicester DiAL HPC [2020225359]
  12. [ACTP238]

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This article discusses the phenomenon of spontaneous scalarization of black holes due to particular couplings between a scalar field and the Gauss-Bonnet invariant, and continues to simulate this phenomenon in the context of binary black hole systems. The authors find two main phenomena: dynamical descalarization and dynamical scalarization, and discuss the observational implications for gravitational-wave tests of general relativity.
Particular couplings between a scalar field and the Gauss-Bonnet invariant lead to spontaneous scalarization of black holes. Here, we continue our work on simulating this phenomenon in the context of binary black hole systems. We consider a negative coupling for which the black-hole spin plays a major role in the scalarization process. We find two main phenomena: (i) dynamical descalarization, in which initially scalarized black holes form an unscalarized remnant, and (ii) dynamical scalarization, whereby the late merger of initially unscalarized black holes can cause scalar hair to grow. An important consequence of the latter case is that modifications to the gravitational waveform due to the scalar field may only occur postmerger, as its presence is hidden during the entirety of the inspiral. However, with a sufficiently strong coupling, we find that scalarization can occur before the remnant has even formed. We close with a discussion of observational implications for gravitational-wave tests of general relativity.

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