Gravitational cubic-in-spin interaction at the next-to-leading post-Newtonian order

TL;DR

This paper derives the complete gravitational cubic-in-spin effective action at the next-to-leading order in the post-Newtonian expansion for generic compact binaries, advancing the understanding of finite-size effects at 4.5PN order.

Contribution

It extends the effective field theory for gravitating spinning objects to include the cubic-in-spin sector at 4.5PN order, the first such completion beyond current 4PN results.

Findings

Complete cubic-in-spin effective action at 4.5PN order.

Highlights differences between even and odd parity sectors.

Provides insights into quantum spin interactions and amplitude factorization.

Abstract

In this work we derive for the first time the complete gravitational cubic-in-spin effective action at the next-to-leading order in the post-Newtonian (PN) expansion for the interaction of generic compact binaries via the effective field theory for gravitating spinning objects, which we extend in this work. This sector, which enters at the fourth and a half PN (4.5PN) order for rapidly-rotating compact objects, completes finite-size effects up to this PN order, and is the first sector completed beyond the current state of the art for generic compact binary dynamics at the 4PN order. At this order in spins with gravitational nonlinearities we have to take into account additional terms, which arise from a new type of worldline couplings, due to the fact that at this order the Tulczyjew gauge for the rotational degrees of freedom, which involves the linear momentum, can no longer be approximated only in terms of the four-velocity. One of the main motivations for us to tackle this sector is also to see what happens when we go to a sector, which corresponds to the gravitational Compton scattering with quantum spins larger than one, and maybe possibly also get an insight on the inability to uniquely fix its amplitude from factorization when spins larger than two are involved. A general observation that we can clearly make already is that even-parity sectors in the order of the spin are easier to handle than odd ones. In the quantum context this corresponds to the greater ease of dealing with bosons compared to fermions.