Corrections to the GW phase in the Fourier space computed within the stationary phase approximation for a quasi-circular binary (see Eq. (12)).
|Mechanism||γ(β = 0)||κ0||γ(β = 1)||κ1|
|Gravitational drag||11/3||− η−3(1 − 3η)π−11∕3||3||− η−16∕5(1 − 3η)π−3|
|Accretion – Bondi||11/3||− η−3(1 − 3η)π−11∕3||3||− η−16∕5(1 − 3η)π−3|
|Accretion – collisionless||3||− η−1π−3||7/3||− η−6∕5π−7∕3|
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