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Octupolar bremsstrahlung waveform up to the two-loop level and the third-and-a-half post-Newtonian accuracy

Published 10 Sep 2026 in gr-qc | (2609.11835v1)

Abstract: Extending our recent work (which focussed on the even-parity quadrupolar part of the waveform), we compute the even-parity octupolar contribution, U3U_3, to the gravitational waveform Wc<sup>4</sup>r4Gmˉ<sup>i</sup>mˉ<sup>j</sup>hijW \equiv \frac{c<sup>4</sup> r}{4G} \bar m<sup>{i}</sup> \bar m<sup>{j</sup> } h_{i j} emitted during the scattering of two masses. We work within the Multipolar Post-Minkowskian (MPM) formalism, and use the 3.5 Post-Newtonian (PN) accurate radiation-reacted quasi-Keplerian representation of the hyperbolic motion. We explicitly evaluate the frequency-domain value U^3(ω,θ,φ)\hat U_3(ω, θ,φ) of U3U_3 up to the 2-loop level, i.e. O(G<sup>4) O(G<sup>4) contributions to hij(ω,θ,φ)h_{ij}(ω, θ,φ), corresponding to O(G<sup>3)O(G<sup>3) contributions to U^3(ω,θ,φ)\hat U_3(ω, θ,φ). As a crucial partial confirmation of our result, we find that the 1-loop truncation of our 3.5 PN frequency-domain MPM waveform agrees with corresponding existing Effective Field Theory (EFT) results when taking into account exactly the {\it same} (2.5PN-level) difference in the definitions of the center-of-mass origins within the two formalisms that was deduced from our previous quadrupolar comparison.

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