Nonlocal-in-time action for the fourth post-Newtonian conservative dynamics of two-body systems
By T. Damour, P. Jaranowski, G. Schāfer. 2014
215 citations recorded by the source corpus.
We complete the analytical determination, at the 4th post-Newtonian (4PN) approximation, of the conservative dynamics of gravitationally interacting two-point-mass systems. This completion is obtained by resolving the infra-red ambiguity which had blocked a previous 4PN calculation [P. Jaranowski and G. Sch\"afer, Phys. Rev. D 87, 081503(R) (2013)] by taking into account the 4PN breakdown of the usual near-zone expansion due to infinite-range tail-transported temporal correlations found long ago [L. Blanchet and T. Damour, Phys. Rev. D 37, 1410 (1988)]. This leads to a Poincar\'e-invariant 4PN-accurate effective action for two masses, which mixes instantaneous interaction terms (described by a usual Hamiltonian) with a (time-symmetric) nonlocal-in-time interaction.
Subfields: Astronomy and Astrophysics, Atomic and Molecular Physics, and Optics
View Paper: https://www.semanticscholar.org/paper/3bbe98b44befdc47c24291b8776bff2130dd790d
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Citations in the corpus
- Spinning black hole binary dynamics, scattering amplitudes, and effective field theory (2020, methodology): “In the inspiral phase, we have the traditional post-Newtonian (PN) approximation using methods in classical gravity [5, 6] and the nonrelativistic general relativity (NRGR) formalism [7, 8] based on effective field theory (EFT), as well as the post-Minkowskian (PM) expansion [9–17].”
- Classical black hole scattering from a worldline quantum field theory (2020, background): “The state of the art is 4PN level for the potential [22–32], parts of 5PN [33–35] and 6PN [36–41], and 3PN [42–44] for the gravitational radiation emitted from a quasi-circular inspiral (see also ref.”
- Post-Minkowskian effective field theory for conservative binary dynamics (2020, methodology): “As a result, joining an effort which involves also more ‘traditional’ methods [18–24], the present state-of-the-art in NRGR is at the fourth PN (4PN) order of accuracy in the conservative sector for non-spinning bodies [8, 17, 25– 31], which includes also contributions induced from (conservative) ra”
- Spinning gravitating objects in the effective field theory in the post-Newtonian scheme (2015, background): “5PN order, should be obtained at least to 4PN order, which was recently completed in the non-spinning case [9].”
- Gravitational scattering, post-Minkowskian approximation, and effective-one-body theory (2016, background): “Therefore, the exact computation of a certain term in the PM expansion of χ (as we shall report below) represents an information about the two-body dynamics which goes beyond all the present PN knowledge (which is limited to the 4PN level [36], [30]), though it evidently misses some of the informati”
- Black hole binary dynamics from the double copy and effective theory (2019, background): “sformations, which we solved up to 4PN order. Given the canonical transformation built above, the remaining free coecients can be adjusted to obtain a perfect match between H4PN in Eq.(8.41) of Ref. [35,36] and our result in Eq. (10.8), H4PN(R;P) O(G3v4) = H3PM(r;p) O(G3v4) ; (11.6) valid up to O(G3”
- High-energy gravitational scattering and the general relativistic two-body problem (2017, methodology): “The conservative two-body dynamics was derived, successively, at the second post-Newtonian (2PN) [14, 15], third postNewtonian (3PN) [16], and fourth post-Newtonian (4PN) [17] levels (with a crucial 4PN contribution having been derived by black-hole perturbation theory [18]).”
- The Effective Field Theorist's Approach to Gravitational Dynamics (2016, background): “) At 4PN order we also find time non-locality in the effective action, due to hereditary effects [111, 112].”
- From boundary data to bound states (2019, methodology): “Using the powerful EFT machinery, as well as other methodologies [15–18], the current level of accuracy in the PN framework has achieved the next-tonext-to-next-to-next-to-leading order (N4LO) in the conservative sector, or four-loops [19–23], and up to five-loops in the static limit [24, 25].”