pith. sign in

arxiv: 2604.10654 · v1 · submitted 2026-04-12 · 🌀 gr-qc

Post-Newtonian dynamics of charged compact binaries

Pith reviewed 2026-05-10 16:30 UTC · model grok-4.3

classification 🌀 gr-qc
keywords post-Newtonian approximationcharged compact binariesgravitational radiationelectromagnetic radiationinspiral dynamicsflux balance equationEinstein-Maxwell theorymultipole moments
0
0 comments X

The pith

The orbital angular frequency of quasi-circular charged compact binaries evolves according to combined gravitational and electromagnetic radiation fluxes computed to next-to-leading order.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines dissipative dynamics of compact binary systems that carry electric charge in Einstein-Maxwell theory. It evaluates the mass and electric multipole moments to obtain the total radiation fluxes in gravity and electromagnetism at the next-to-leading post-Newtonian order. These fluxes enter the balance equation to yield the time evolution of orbital angular frequency during quasi-circular inspirals. The work also checks stability conditions for circular orbits and shows how varying charge-to-mass ratios modify the inspiral behavior.

Core claim

By evaluating the mass and electric multipole moments of binaries, the combined gravitational and electromagnetic radiation fluxes are computed to the next-to-leading order. Using the flux balance equation, the evolution of the orbital angular frequency is obtained for quasi-circular inspirals. The analysis further determines the stability of circular orbits in charged black hole binaries and the dependence of inspiral dynamics on different charge-to-mass ratios.

What carries the argument

Mass and electric multipole moments of the binary that enter the calculation of combined gravitational and electromagnetic radiation fluxes, together with the flux balance equation that determines the orbital frequency evolution.

If this is right

  • The rate of increase in orbital frequency during inspiral depends explicitly on the charge-to-mass ratios of each body.
  • Stability of circular orbits receives electromagnetic corrections that can alter the range of allowed separations compared with neutral binaries.
  • The total energy flux includes an electromagnetic contribution that accelerates the inspiral relative to the purely gravitational case.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Waveform models for binary mergers would need to incorporate charge-dependent frequency evolution to avoid systematic errors in parameter estimation.
  • Comparison of observed inspiral rates against neutral templates could place observational bounds on possible charge-to-mass ratios in compact objects.

Load-bearing premise

The post-Newtonian expansion remains valid and the binaries stay in quasi-circular orbits while their charge-to-mass ratios act as fixed free parameters.

What would settle it

A measurement of the orbital frequency derivative in a binary with independently determined charge-to-mass ratios that fails to match the rate predicted by balancing the computed gravitational plus electromagnetic energy loss.

Figures

Figures reproduced from arXiv: 2604.10654 by Shuai Zhang, Tan Liu, Zi-Han Zhang, Zong-Kuan Guo.

Figure 1
Figure 1. Figure 1: FIG. 1. The PN ISCO of a charged binary. The black dotted [PITH_FULL_IMAGE:figures/full_fig_p011_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. The contributions of different PN orders to the EM [PITH_FULL_IMAGE:figures/full_fig_p012_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. The total radiation of Case.(c) binary compares to [PITH_FULL_IMAGE:figures/full_fig_p012_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. The evolution of the GW frequency of Case.(c) binary compares to the Case.(a) binary. For a binary [PITH_FULL_IMAGE:figures/full_fig_p013_5.png] view at source ↗
read the original abstract

We investigate the dissipative dynamics of compact binary systems within the framework of Einstein-Maxwell theory. By evaluating the mass and electric multipole moments of binaries, we compute the combined gravitational and electromagnetic radiation fluxes to the next-to-leading order. Using the flux balance equation, we obtain the evolution of the orbital angular frequency for quasi-circular inspirals. We further analyze the stability of circular orbits in charged black hole binaries and assess how different charge-to-mass ratios affect the inspiral dynamics.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 3 minor

Summary. The manuscript claims to extend post-Newtonian methods to charged compact binaries in Einstein-Maxwell theory by calculating mass and electric multipole moments, deriving combined gravitational and electromagnetic radiation fluxes at next-to-leading order, and inserting these into the flux-balance law to obtain the orbital angular frequency evolution for quasi-circular inspirals. It additionally analyzes the stability of circular orbits for varying charge-to-mass ratios.

Significance. If the calculations are accurate, the work supplies analytic expressions for frequency evolution that incorporate electromagnetic radiation losses, extending standard PN techniques in a consistent manner. This could serve as a reference for waveform modeling or stability studies in charged systems, though the astrophysical relevance of non-negligible charges remains limited. The reliance on established multipole and flux-balance methods is a strength.

major comments (1)
  1. The central frequency-evolution result relies on fluxes truncated at next-to-leading order, yet the manuscript provides no explicit error estimates or bounds on neglected higher-order terms and their effect on the orbital-frequency derivative; this directly impacts the claimed precision of the evolution equation.
minor comments (3)
  1. The notation for electric multipole moments should be defined more explicitly and compared to the neutral limit to aid readability and verification.
  2. The stability analysis of circular orbits would be strengthened by a direct quantitative comparison (e.g., shift in innermost stable orbit radius) to the uncharged case.
  3. The introduction would benefit from additional references to prior PN work on neutral binaries and Einstein-Maxwell multipole expansions for context.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback on our manuscript. We address the single major comment below and have revised the text to incorporate an explicit discussion of truncation errors.

read point-by-point responses
  1. Referee: The central frequency-evolution result relies on fluxes truncated at next-to-leading order, yet the manuscript provides no explicit error estimates or bounds on neglected higher-order terms and their effect on the orbital-frequency derivative; this directly impacts the claimed precision of the evolution equation.

    Authors: We agree that an explicit statement on truncation error strengthens the presentation. In the revised manuscript we have added a paragraph (now in Section 5) noting that the neglected terms in the combined gravitational and electromagnetic fluxes enter at O((v/c)^4) relative to the next-to-leading-order contributions. Consequently, the relative error induced in dΩ/dt scales as O((v/c)^4) and remains ≲ 3 % for the orbital velocities v/c ≲ 0.25 relevant to the late inspiral regime we consider. This estimate follows directly from the standard post-Newtonian ordering already used for the multipole moments and fluxes; a complete next-to-next-to-leading-order calculation lies beyond the scope of the present work. revision: yes

Circularity Check

0 steps flagged

No significant circularity; derivation extends standard PN multipole formalism independently

full rationale

The paper computes mass and electric multipole moments for charged binaries in Einstein-Maxwell theory, derives combined gravitational and electromagnetic radiation fluxes to next-to-leading order, and inserts them into the standard flux-balance law to obtain orbital-frequency evolution for quasi-circular inspirals. These steps follow the established post-Newtonian multipole expansion and energy-balance procedure without fitting any parameters to the paper's own outputs, without renaming known results as new predictions, and without load-bearing self-citations that reduce the central claim to prior work by the same authors. The charge-to-mass ratios are treated as free parameters, and the derivation remains self-contained against external PN benchmarks.

Axiom & Free-Parameter Ledger

1 free parameters · 2 axioms · 0 invented entities

The central claim rests on the validity of the post-Newtonian expansion in Einstein-Maxwell theory and the applicability of the flux-balance equation to dissipative dynamics; no new entities are introduced.

free parameters (1)
  • charge-to-mass ratio
    Treated as a variable parameter to assess effects on inspiral and stability; not fitted to data but explored for different values.
axioms (2)
  • domain assumption Post-Newtonian approximation is valid for the dissipative dynamics of the binary
    Invoked to compute multipole moments and radiation fluxes to NLO.
  • domain assumption Quasi-circular orbits are maintained during the inspiral phase
    Used to derive the orbital angular frequency evolution.

pith-pipeline@v0.9.0 · 5367 in / 1350 out tokens · 49366 ms · 2026-05-10T16:30:24.787262+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

56 extracted references · 56 canonical work pages

  1. [1]

    +O(Q 2) +O(c −4).(130) 11 This equation is under an expanded conditionQ≪M,ζ 0 ≪1 andQ ≪1. Ifq B ≪q A, we haveZ∼1 andQ ≪ζ 0, which is consistent with the angular frequency parameter of a neutral test particle on the RN metric as xIRN = 1 6 1 + 1 6 Q2 M2 +O Q M 4 .(131) which is calculated in appendix.C. Using the relationship in Eq.(80) and Eq.(82) in the ...

  2. [2]

    B. P. Abbott and et al (LIGO Scientific Collaboration and Virgo Collaboration), Phys. Rev. Lett.116, 061102 (2016)

  3. [3]

    B. P. Abbott and et al. (LIGO Scientific Collaboration and Virgo Collaboration), Phys. Rev. Lett.116, 241103 (2016)

  4. [4]

    B. P. Abbott and et al, Phys. Rev. Lett.118, 221101 (2017)

  5. [5]

    B. P. Abbott and et al. (LIGO Scientific Collaboration and Virgo Collaboration), Phys. Rev. Lett.119, 141101 (2017)

  6. [6]

    Abbott and et al

    R. Abbott and et al. (LIGO Scientific Collaboration and Virgo Collaboration), Phys. Rev. Lett.125, 101102 (2020)

  7. [7]

    R. P. Kerr, Phys. Rev. Lett.11, 237 (1963)

  8. [8]

    E. T. Newman, E. Couch, K. Chinnapared, A. Exton, A. Prakash, and R. Torrence, Journal of Mathematical Physics6, 918 (1965)

  9. [9]

    Zajaˇ cek, A

    M. Zajaˇ cek, A. Tursunov, A. Eckart, and S. Britzen, Monthly Notices of the Royal Astronomical Society480, 4408 (2018), https://academic.oup.com/mnras/article- pdf/480/4/4408/25539563/sty2182.pdf

  10. [10]

    Zajaˇ cek, A

    M. Zajaˇ cek, A. Tursunov, A. Eckart, S. Britzen, E. Hack- mann, V. Karas, Z. Stuchl´ ık, B. Czerny, and J. A. Zen- sus, Journal of Physics: Conference Series1258, 012031 (2019)

  11. [11]

    Gu, H.-T

    H.-P. Gu, H.-T. Wang, and L. Shao, Phys. Rev. D109, 024058 (2024)

  12. [12]

    G. W. Gibbons, Communications in Mathematical Physics44, 245 (1975). 23

  13. [13]

    Y. Gong, Z. Cao, H. Gao, and B. Zhang, Monthly Notices of the Royal Astronomical Society488, 2722 (2019), https://academic.oup.com/mnras/article- pdf/488/2/2722/29002740/stz1904.pdf

  14. [14]

    Cardoso, C

    V. Cardoso, C. F. Macedo, P. Pani, and V. Ferrari, Jour- nal of Cosmology and Astroparticle Physics2016, 054 (2016)

  15. [15]

    Sasaki, T

    M. Sasaki, T. Suyama, T. Tanaka, and S. Yokoyama, Phys. Rev. Lett.117, 061101 (2016)

  16. [16]

    Ali-Ha¨ ımoud, E

    Y. Ali-Ha¨ ımoud, E. D. Kovetz, and M. Kamionkowski, Phys. Rev. D96, 123523 (2017)

  17. [17]

    Chen and Q.-G

    Z.-C. Chen and Q.-G. Huang, The Astrophysical Journal 864, 61 (2018)

  18. [18]

    Henry, F

    Q. Henry, F. m. c. Larrouturou, and C. Le Poncin- Lafitte, Phys. Rev. D108, 024020 (2023)

  19. [19]

    Henry, F

    Q. Henry, F. m. c. Larrouturou, and C. Le Poncin- Lafitte, Phys. Rev. D109, 084048 (2024)

  20. [20]

    Placidi, E

    A. Placidi, E. Grilli, M. Orselli, M. Pegorin, N. Bar- tolo, and P. Mastrolia, “Charged black-hole binary evolution at second post-newtonian order,” (2025), arXiv:2509.20432 [hep-th]

  21. [21]

    Khalil, N

    M. Khalil, N. Sennett, J. Steinhoff, J. Vines, and A. Buo- nanno, Phys. Rev. D98, 104010 (2018)

  22. [22]

    Inspiraling binary charged black holes in an external magnetic field: Appli- cation of post-newtonian dynamics in einstein-maxwell theory,

    R. Tang, L. Liu, and W.-B. Han, “Inspiraling binary charged black holes in an external magnetic field: Appli- cation of post-newtonian dynamics in einstein-maxwell theory,” (2025), arXiv:2512.04806 [gr-qc]

  23. [23]

    B. P. Abbott and et al. (LIGO Scientific Collaboration and Virgo Collaboration), Phys. Rev. Lett.119, 161101 (2017)

  24. [24]

    Landau and E

    L. Landau and E. Lifshitz,The classical theory of fields, Vol. 2 (Pergamon Press, Oxford; New York, 1971)

  25. [25]

    Blanchet, Living Reviews in Relativity27, 4 (2024)

    L. Blanchet, Living Reviews in Relativity27, 4 (2024)

  26. [26]

    Blanchet and G

    L. Blanchet and G. Faye, Journal of Mathematical Physics41, 7675–7714 (2000)

  27. [27]

    Damour and G

    T. Damour and G. Sch¨ afer, General Relativity and Grav- itation17, 879 (1985)

  28. [28]

    Bernard, L

    L. Bernard, L. Blanchet, A. Boh´ e, G. Faye, and S. Marsat, Phys. Rev. D93, 084037 (2016)

  29. [29]

    J. D. Jackson,Classical Electrodynamics, 3rd ed. (Wiley, New York, 1998)

  30. [30]

    Polonyi, Annals of Physics342, 239 (2014)

    J. Polonyi, Annals of Physics342, 239 (2014)

  31. [31]

    Blanchet and B

    L. Blanchet and B. R. Iyer, Classical and Quantum Grav- ity20, 755 (2003)

  32. [32]

    Maggiore,Gravitational Waves

    M. Maggiore,Gravitational Waves. Vol. 1: Theory and Experiments(Oxford University Press, 2007)

  33. [33]

    Poisson and C

    E. Poisson and C. M. Will,Gravity(Cambridge Univer- sity Press, 2014)

  34. [34]

    Blanchet, Phys

    L. Blanchet, Phys. Rev. D47, 4392 (1993)

  35. [35]

    L. Liu, Ø. Christiansen, Z.-K. Guo, R.-G. Cai, and S. P. Kim, Phys. Rev. D102, 103520 (2020)

  36. [36]

    C. W. Lincoln and C. M. Will, Phys. Rev. D42, 1123 (1990)

  37. [37]

    L. Liu, Ø. Christiansen, W.-H. Ruan, Z.-K. Guo, R.-G. Cai, and S. P. Kim, The European Physical Journal C 81, 1048 (2021)

  38. [38]

    Blanchet and G

    L. Blanchet and G. Faye, Classical and Quantum Gravity 36, 085003 (2019)

  39. [39]

    Damour and B

    T. Damour and B. R. Iyer, Phys. Rev. D43, 3259 (1991)

  40. [40]

    Blanchet and G

    L. Blanchet and G. Schaefer, MNRAS239, 845 (1989)

  41. [41]

    Pugliese, H

    D. Pugliese, H. Quevedo, and R. Ruffini, Phys. Rev. D 88, 024042 (2013)

  42. [42]

    Pugliese, H

    D. Pugliese, H. Quevedo, and R. Ruffini, Phys. Rev. D 83, 104052 (2011)

  43. [43]

    Levin and G

    J. Levin and G. Perez-Giz, Phys. Rev. D77, 103005 (2008)

  44. [44]

    Chandrasekhar,The Mathematical Theory of Black Holes(Oxford University Press, 1998)

    S. Chandrasekhar,The Mathematical Theory of Black Holes(Oxford University Press, 1998)

  45. [45]

    V. C. de Andrade, L. Blanchet, and G. Faye, Classical and Quantum Gravity18, 753 (2001)

  46. [46]

    Jaranowski and G

    P. Jaranowski and G. Sch¨ afer, Phys. Rev. D57, 7274 (1998)

  47. [47]

    Damour, P

    T. Damour, P. Jaranowski, and G. Sch¨ afer, Phys. Rev. D62, 084011 (2000)

  48. [48]

    L. E. Kidder, C. M. Will, and A. G. Wiseman, Phys. Rev. D47, 3281 (1993)

  49. [49]

    Blanchet, D

    L. Blanchet, D. Langlois, and E. Ligout, Phys. Rev. D 112, 064025 (2025)

  50. [50]

    B. R. Iyer and C. M. Will, Phys. Rev. Lett.70, 113 (1993)

  51. [51]

    Blanchet and T

    L. Blanchet and T. Damour, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences320, 379 (1986)

  52. [52]

    J. D. Jackson,Classical Electrodynamics(John Wiley & Sons, 1999)

  53. [53]

    Blanchet, G

    L. Blanchet, G. Faye, and B. Ponsot, Phys. Rev. D58, 124002 (1998)

  54. [54]

    K. S. Thorne, Rev. Mod. Phys.52, 299 (1980)

  55. [55]

    Ross, Phys

    A. Ross, Phys. Rev. D85, 125033 (2012)

  56. [56]

    A. G. Wiseman, Phys. Rev. D46, 1517 (1992)