We recommend starting with this manual (ver. 2021-12-11) that contains naming conventions across the BHPC data below.
!! INFORMATION !! (Update: 2025-09-01) We've fixed a few minor errors and typos in the old 5PNe10 generic-orbit date released here. Please use the updated data set that has '250407' (for fluxes) and '250822' (for Teukolsky amplitudes) in the file names. We're really sorry for any problems these mistakes might cause; the results in arXiv:2008.13554 and arXiv:2111.05288 have basically stayed the same. If you have any questions about our dataset at all, please get in touch with bhpc1996_at_gmail.com and we'll be happy to help!
Extreme mass ratio inspirals on the equatorial plane in the adiabatic order
Phys. Rev. D 102, 064005 (2020), arXiv:2008.13554
5PNe10 (but arbitrary inclination) generic fluxes in Kerr (last updated on April 7, 2025): Maple data, Mathematica data
Calculation of radiation reaction effect on orbital parameters in Kerr spacetime
Prog. Theor. Exp. Phys. 2015, 073E03 (2015) , arXiv:1505.01600
4PN e6 (but arbitrary inclination) generic fluxes in Kerr (last updated on August 21, 2020): Maple data, Mathematica data
Gravitational waves from a particle in circular orbits around a rotating black hole to the 11th post-Newtonian order
Prog. Theor. Exp. Phys. 2015, Issue 3, 033E01 (2015), arXiv:1412.5689
11PN equatorial-circular fluxes in Kerr (last updated on March 11, 2015): Maple data, Mathematica data
Gravitational Waves from a Particle in Circular Orbits around a Schwarzschild Black Hole to the 22nd Post-Newtonian Order
Prog.Theor.Phys.128, 971-992 (2012), arXiv:1211.5535
22PN circular fluxes in Schwarzschild (last updated on November 19, 2012): Maple data, Mathematica data
NOTE: the asymptotic mode amplitude "Zlm" in the case of circular and equatorial orbits can be also reconstructed from `rho[l, m]' and `delta[l, m]' of (so named) PN factorized multipolar waveforms. They are presented through 22PN (Schwarzschild) and 11PN (Kerr) order in above Maple/Mathematica files for fluxes. See README therein for details, and Sec.4.2.1. and 4.2.2. of Fujita's 11PN paper [arXiv:1412.5689] for our BHPC convention.
Adiabatic waveforms from extreme-mass-ratio inspirals: an analytical approach
Phys. Rev. Lett 128 (2021) 23, 231101, arXiv:2111.05288
(a omega)^3 Spheroidal harmonics (s = -2), and 5PNe10 (but arbitrary inclination) generic mode amplitudes in Kerr (last updated on September 1, 2025): Maple data, Mathematica data (18MB).
Post-Newtonian templates for phase evolution of spherical extreme mass ratio inspirals
Phys.Rev.D 111 (2025) 6, 064043, arXiv:2411.09147
12PN (but arbitrary inclination) spherical fluxes in Kerr, TaylorT families and TaylorF2 templates for Kerr spherical inspirals (last updated on November 15, 2024): Maple data
Extreme mass ratio inspirals on the equatorial plane in the adiabatic order
Phys. Rev. D 102, 064005 (2020), arXiv:2008.13554
Equatorial fluxes in Kerr (last updated on August 31, 2020): Numerical data (17MB)
Coming soon! [If you're interested in the generic data (fluxes and amplitudes), please get in touch with bhpc1996_at_gmail.com and we'll do our very best to help!]
The averaged rate of change of the orbital angular momentum and Carter constant due to tidal resonances
Importance of tidal resonances in extreme-mass-ratio inspirals
Phys.Rev.D 104, 044056 (2021), arXiv:2104.03422
For (n : k : m) = (3 : 0 : -2), (3 : -4 : 2), (3 : 0 : 2) and (3 : -4 : -2) (last updated on July 26, 2021): Fittings Tidal Resonances.wl (Mathematica)
Modeling transient resonances in extreme-mass-ratio inspirals
Phys.Rev.D 106 (2022) 10, 104001 arXiv:2205.04808
For (n : k : m) = (-3 : 1 : 1), (-3 : 2 : 0), (-3 : 3 : -1), (-4 : 1 : 1), (-4 : 2 : 0) and (-4 : 3 : -1) (last updated on August 14, 2022): Fittings Tidal Resonances-m01.wl (Mathematica)