2013
DOI: 10.1103/physrevd.87.124036
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Effective-one-body Hamiltonian with next-to-leading order spin-spin coupling for two nonprecessing black holes with aligned spins

Abstract: The canonical Arnowitt-Deser-Misner (ADM) Hamiltonian with next-to-leading order spin-spin coupling [J. Steinhoff, S. Hergt, and G. Schäfer, Phys. Rev. D 77, 081501 (2008); 78, 101503 (2008)] is converted into the effective-one-body (EOB) formalism of [T. Damour, P. Jaranowski, and G. Schäfer, Phys. Rev. D 78, 024009 (2008)] for the special case of spinning black hole binaries whose spins are aligned with the angular momentum. In particular, we propose to include the new terms by adding a dynamical term of nex… Show more

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Cited by 24 publications
(13 citation statements)
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“…Identifying the various powers of u andâ on both sides of Eq. (2.22) allows one to convert our analytical results (3.10)-(3.11) into an analytical knowledge of the PN expansions of f (n)resc A (u) and δG (n)resc S (u) (with n = 0, 2), with the following results: The only terms among the above, high-accuracy, PN expansions that were known from standard PN compu-tations were the next-to-leading-order (NLO) corrections to δG (0)resc S (i.e., 1 + 102 5 u) [57,58] and to f (0)resc A (u) (i.e., 1 + 11 4 u) [59].…”
Section: Analytical Computation Of the Self-force Corrections To mentioning
confidence: 99%
“…Identifying the various powers of u andâ on both sides of Eq. (2.22) allows one to convert our analytical results (3.10)-(3.11) into an analytical knowledge of the PN expansions of f (n)resc A (u) and δG (n)resc S (u) (with n = 0, 2), with the following results: The only terms among the above, high-accuracy, PN expansions that were known from standard PN compu-tations were the next-to-leading-order (NLO) corrections to δG (0)resc S (i.e., 1 + 102 5 u) [57,58] and to f (0)resc A (u) (i.e., 1 + 11 4 u) [59].…”
Section: Analytical Computation Of the Self-force Corrections To mentioning
confidence: 99%
“…[33,[45][46][47]94,134,412,414,415,513,514], and one by T. Damour, A. Nagar, and their collaborators, e.g. [40,70,143,149,150,154,158,158,159,[161][162][163]381,391,393,396,398,399]. These BBH EOB models both reproduce the PN and test-mass results in the appropriate limits, use the same energy mapping to the effective phase spaces, and the effective description of a test particle in an effective spacetime.…”
Section: Tidal Effective-one-body Models For Binary Inspiralsmentioning
confidence: 91%
“…The chirping signals emitted by inspiraling binaries contain a range of frequency components: if the graviton has mass, the components propagate at different speeds, again given by Eq. (44). This effect can be modeled in the templates used to search for binary signals by including a λ g dependence in the waveform phasing [470].…”
Section: Tests Of Gravitational-wave Propagationmentioning
confidence: 99%