2019
DOI: 10.1007/978-3-030-04260-8_4
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Rotating Black Holes

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“…We now consider the transformation laws for the charges under allowed diffeomorphisms. According to general results [58,59], the change δ ξ Q χ in a conserved and integrable charge Q χ under an allowed infinitesimal diffeomorphism ξ is antisymmetric under ξ ↔ χ and in fact defines a Lie bracket 14 The charges obey the same BMS algebra of the generators, 12 In comparison, this linearity breaks down on t = const slices in the electromagnetic case, where field interaction energy makes a contribution to the mass moment, even at late times [15]. 13 The analytic continuation of the second counter-term S (k) in (4.36) of [31] does not contribute to the charges.…”
Section: Conserved Chargesmentioning
confidence: 99%
“…We now consider the transformation laws for the charges under allowed diffeomorphisms. According to general results [58,59], the change δ ξ Q χ in a conserved and integrable charge Q χ under an allowed infinitesimal diffeomorphism ξ is antisymmetric under ξ ↔ χ and in fact defines a Lie bracket 14 The charges obey the same BMS algebra of the generators, 12 In comparison, this linearity breaks down on t = const slices in the electromagnetic case, where field interaction energy makes a contribution to the mass moment, even at late times [15]. 13 The analytic continuation of the second counter-term S (k) in (4.36) of [31] does not contribute to the charges.…”
Section: Conserved Chargesmentioning
confidence: 99%