Classical spin transitions and absorptive scattering

A bstract We describe an on-shell, amplitudes-based approach to incorporating radiation absorption effects in the post-Minkowskian scattering of generic, compact, spinning bodies. Classical spinning observables are recovered by extrapolating to large spin, results calculated with finite quantum spin- s particles using the properties of spin universality and Casimir interpolation. At leading-order our results give a completely general and non-redundant parametrization of absorptive observables in terms of a finite number of Wilson coefficients associated with 3-particle mass and spin-magnitude changing on-shell amplitudes. We denote these semi-fictitious microscopic processes: classical spin transitions . Explicit results for the leading-order impulse due to the absorption of scalar, electromagnetic and gravitational radiation, for spin transitions ∆ s = 0, ±1, ±2 are given in a fully interpolated form up to $$ \mathcal{O}\left({S}^2\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mfenced> </mml:math> , and Casimir independent contributions given up to $$ \mathcal{O}\left({S}^4\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:mfenced> </mml:math> . Our explicit results reveal some surprising universal patterns. We find that, up to identification of Wilson coefficients, the Casimir independent contributions to the impulse for spinning-up and spinning-down by the same magnitude |∆ s | are identical. For processes where the quantum ∆ s &lt; 0 transition is forbidden, the corresponding classical observable is suppressed in powers of S by a predictable amount. Additionally we find that, while for generic non-aligned spin configurations there is a non-zero scattering angle at leading-order, for aligned spin, similar to non-spinning absorption, the scattering angle vanishes and the impulse is purely longitudinal. The formalism and results presented provide a significant extension of the amplitudes-based calculational pipeline for gravitational waveforms from binary black hole and neutron star systems beyond the point-particle approximation.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-04-23
DOI
https://doi.org/10.1007/jhep04(2026)186
Primary Topic
Quantum Electrodynamics and Casimir Effect
Type
article
Field-Weighted Citation Impact
0.00

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article

Classical spin transitions and absorptive scattering

Juan Pablo Gatica, Callum R. T. Jones
Journal of High Energy Physics
Quantum Electrodynamics and Casimir Effect
article

Classical spin transitions and absorptive scattering

Juan Pablo Gatica, Callum R. T. Jones
article en

Abstract

A bstract We describe an on-shell, amplitudes-based approach to incorporating radiation absorption effects in the post-Minkowskian scattering of generic, compact, spinning bodies. Classical spinning observables are recovered by extrapolating to large spin, results calculated with finite quantum spin- s particles using the properties of spin universality and Casimir interpolation. At leading-order our results give a completely general and non-redundant parametrization of absorptive observables in terms of a finite number of Wilson coefficients associated with 3-particle mass and spin-magnitude changing on-shell amplitudes. We denote these semi-fictitious microscopic processes: classical spin transitions . Explicit results for the leading-order impulse due to the absorption of scalar, electromagnetic and gravitational radiation, for spin transitions ∆ s = 0, ±1, ±2 are given in a fully interpolated form up to $$ \mathcal{O}\left({S}^2\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mfenced> </mml:math> , and Casimir independent contributions given up to $$ \mathcal{O}\left({S}^4\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> <mml:mfenced> <mml:msup> <mml:mi>S</mml:mi> <mml:mn>4</mml:mn> </mml:msup> </mml:mfenced> </mml:math> . Our explicit results reveal some surprising universal patterns. We find that, up to identification of Wilson coefficients, the Casimir independent contributions to the impulse for spinning-up and spinning-down by the same magnitude |∆ s | are identical. For processes where the quantum ∆ s &lt; 0 transition is forbidden, the corresponding classical observable is suppressed in powers of S by a predictable amount. Additionally we find that, while for generic non-aligned spin configurations there is a non-zero scattering angle at leading-order, for aligned spin, similar to non-spinning absorption, the scattering angle vanishes and the impulse is purely longitudinal. The formalism and results presented provide a significant extension of the amplitudes-based calculational pipeline for gravitational waveforms from binary black hole and neutron star systems beyond the point-particle approximation.

Journal of High Energy PhysicsVol. 2026(4)
University of Arizona (US), University of California, Los Angeles (US)
U.S. Department of Energy
Openalex Percentile: Top 98%
Quantum Electrodynamics and Casimir Effect
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