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New Black Hole Solutions in Brans-Dicke Theory of Gravity
General Relativity and Quantum Cosmology · Submitted 4 Nov 1998
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Namely, working directly with the known explicit spacetime solutions in Brans-Dicke theory, it is found that non-trivial Kerr-Newman-type black hole solutions different from general relativistic solutions could occur for the generic Brans-Dicke parameter values -5/2\leq \omega <-3/2.
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The abstract, sentence by sentence
Existence check of non-trivial, stationary axisymmetric black hole solutions in Brans-Dicke theory of gravity in different direction from those of Penrose, Thorne and Dykla, and Hawking is performed. Namely, working directly with the known explicit spacetime solutions in Brans-Dicke theory, it is found that non-trivial Kerr-Newman-type black hole solutions different from general relativistic solutions could occur for the generic Brans-Dicke parameter values -5/2\leq \omega <-3/2. Finally, issues like whether these new black holes carry scalar hair and can really arise in nature and if they can, what the associated physical implications would be are discussed carefully.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Existence check of non-trivial, stationary axisymmetric black hole solutions in Brans-Dicke theory of gravity in different direction from those of Penrose, Thorne and Dykla, and Hawking is performed. | contribution 0.93 | 0.87 | 0.09 | asserted 0.85 |
| s1 | Namely, working directly with the known explicit spacetime solutions in Brans-Dicke theory, it is found that non-trivial Kerr-Newman-type black hole solutions different from general relativistic solutions could occur for the generic Brans-Dicke parameter values -5/2\leq \omega <-3/2. | result 0.97 | 0.95 | 0.87 | hedged possibility 0.78 |
| s2 | Finally, issues like whether these new black holes carry scalar hair and can really arise in nature and if they can, what the associated physical implications would be are discussed carefully. | interpretation 0.74 | 0.70 | 0.06 | unclear 0.71 |
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The paper
Original abstract
Existence check of non-trivial, stationary axisymmetric black hole solutions in Brans-Dicke theory of gravity in different direction from those of Penrose, Thorne and Dykla, and Hawking is performed. Namely, working directly with the known explicit spacetime solutions in Brans-Dicke theory, it is found that non-trivial Kerr-Newman-type black hole solutions different from general relativistic solutions could occur for the generic Brans-Dicke parameter values -5/2\leq \omega <-3/2. Finally, issues like whether these new black holes carry scalar hair and can really arise in nature and if they can, what the associated physical implications would be are discussed carefully.
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References
How the literature uses it
9 arXiv papers cite this in 14 sentences
Papers citing it · 9 sentences without a confident label
Cites it as background 5 papers
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Zaslavskii [ref] generalized the particle collision with the unbounded center-of-mass energy and classified particle collisions with arbitrary high center-of-mass energy near the GMGHS black hole [ref] , near a black hole in Brans-Dicke theory [ref] investigated by Sultana and Bose [ref] , and near naked singularities in a Fisher spacetime or a Janis-Newman-Winicour spacetime [ref] investigated by Patil and Joshi [ref] , into the same class.
Neutral particle collisions near Gibbons-Maeda-Garfinkle-Horowitz-Strominger black holes after shadow observations · Introduction · 0.87
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In the Brans-Dicke theory an exact solution is known (see [ref] and references therein):
High energy particle collisions and geometry of horizon · Black hole in Brans-Dicke theory · 0.83
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Attempts to construct a rotating solution (and solutions with NUT) were also made in the framework of the Brans-Dicke (BD) theory [ref] .
Photon surfaces, shadows and accretion disks in gravity with minimally coupled scalar field · Introduction · 0.98
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