4.4 Article

Responses of the Brans-Dicke field due to gravitational collapses

期刊

CLASSICAL AND QUANTUM GRAVITY
卷 27, 期 20, 页码 -

出版社

IOP Publishing Ltd
DOI: 10.1088/0264-9381/27/20/205002

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资金

  1. Korean government (MOEHRD) [KRF-313-2007-C00164, KRF-341-2007-C00010]
  2. BK21
  3. Ministry of Education, Science & Technology (MoST), Republic of Korea [KAIST_HR_2010_32] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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We study responses of the Brans-Dicke field due to gravitational collapses of scalar field pulses using numerical simulations. Double-null formalism is employed to implement the numerical simulations. If we supply a scalar field pulse, it will asymptotically form a black hole via dynamical interactions of the Brans-Dicke field. Hence, we can observe the responses of the Brans-Dicke field by two different regions. First, we observe the late time behaviors after the gravitational collapse, which include formations of a singularity and an apparent horizon. Second, we observe the fully dynamical behaviors during the gravitational collapse and view the energy-momentum tensor components. For the late time behaviors, if the Brans-Dicke coupling is greater (or smaller) than -1.5, the Brans-Dicke field decreases (or increases) during the gravitational collapse. Since the Brans-Dicke field should be relaxed to the asymptotic value with the elapse of time, the final apparent horizon becomes time-like (or space-like). For the dynamical behaviors, we observed the energy-momentum tensors around omega similar to -1.5. If the Brans-Dicke coupling is greater than -1.5, the T-uu component can be negative at the outside of the black hole. This can allow an instantaneous inflating region during the gravitational collapse. If the Brans-Dicke coupling is less than -1.5, the oscillation of the T-vv component allows the apparent horizon to shrink. This allows a combination that violates weak cosmic censorship. Finally, we discuss the implications of the violation of the null energy condition and weak cosmic censorship.

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