We present BHPTNRSur2dq1e3, a reduced order surrogate model of gravitational waves emitted from binary black hole (BBH) systems in the comparable to large mass ratio regime with aligned spin (χ1) on the heavier mass (m1). We trained this model on waveform data generated from point particle black hole perturbation theory (ppBHPT) with mass ratios varying from 3≤q≤1000 and spins from −0.8≤χ1≤0.8. The waveforms are 13,500m1 long and include all spin-weighted spherical harmonic modes up to ℓ=4 except the (4,1) and m=0 modes. We find that for binaries with χ1≲−0.5, retrograde quasi-normal modes are significantly excited, thereby complicating the modeling process. To overcome this issue, we introduce a domain decomposition approach to model the inspiral and merger-ringdown portion of the signal separately. The resulting model can faithfully reproduce ppBHPT waveforms with a median time-domain mismatch error of 8×10−5. We then calibrate our model with numerical relativity (NR) data in the comparable mass regime (3≤q≤10). By comparing with spin-aligned BBH NR simulations at q=15, we find that the dominant quadrupolar (subdominant) modes agree to better than ≈10−3(≈10−2) when using a time-domain mismatch error, where the largest source of calibration error comes from the transition-to-plunge and ringdown approximations of perturbation theory. Mismatch errors are below ≈10−2 for systems with mass ratios between 6≤q≤15 and typically get smaller at larger mass ratio. Our two models - both the ppBHPT waveform model and the NR-calibrated ppBHPT model - will be publicly available through gwsurrogate and the Black Hole Perturbation Toolkit packages.
@article{arxiv.2407.18319,
title = {Gravitational wave surrogate model for spinning, intermediate mass ratio binaries based on perturbation theory and numerical relativity},
author = {Katie Rink and Ritesh Bachhar and Tousif Islam and Nur E. M. Rifat and Kevin Gonzalez-Quesada and Scott E. Field and Gaurav Khanna and Scott A. Hughes and Vijay Varma},
journal= {arXiv preprint arXiv:2407.18319},
year = {2026}
}