We recommend starting with this manual (ver 11/12/2021) that contains naming conventios 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 7 April, 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 21 August 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 11 March 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 19 Nov 2012): Maple data, Mathematica dat
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 01 Sep 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 15 Nov 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 31 August 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 26 July 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 14 August 2022): Fittings Tidal Resonances-m01.wl (Mathematica)