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P., Abbott, R., Abbott, T

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  • background we impose regularity at the horizon and discard the redundant growing mode by setting D1 = 0. This yields a unique solution for D2, proportional to A1. As usual, the ℓ = 2 magnetic LN is determined from the ratio of the O(r−2) term and the O(r3) terms in the asymptotic expansion of the complete metric perturbation h0. To leading order in ϵ, we obtain from Eq. (1.24), kB(up) ℓ=2 = MDMr4 s [5 + 12 log(rs/R)] 3R5 , (3.30) where we have introduced an effective radial scale R, to be discussed later,

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GPU-Accelerated X-ray Pulse Profile Modeling

astro-ph.HE · 2025-10-09 · conditional · novelty 8.0

First public GPU-accelerated pulse-profile modeling code for X-ray millisecond pulsars that delivers 10^3–10^4 speedups to 2–5 ms per evaluation at 10^{-3} relative accuracy and removes an interpolation bias in atmosphere tables.

Revisiting the picture of circumbinary disc truncation

astro-ph.EP · 2026-06-25 · unverdicted · novelty 6.0

Cavity truncation in circumbinary discs is set by binary parameters together with instantaneous cavity eccentricity and relative apsidal orientation, yielding a prescription for pericentre radius Rp and semi-major axis acav.

Tests of scalar polarizations with multi-messenger events

gr-qc · 2026-04-27 · conditional · novelty 6.0

Adding the electromagnetic polarization-angle prior to a PPE test of GW170817 tightens the scalar-breathing amplitude bound by ~60% and yields a non-significant ~2–3σ preference for a scalar mode.

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