pith. machine review for the scientific record. sign in

arxiv: 2604.20975 · v1 · submitted 2026-04-22 · 🌌 astro-ph.HE · gr-qc

Recognition: unknown

Probing Supermassive Black Hole Mergers with Pulsar Timing Arrays

Hippolyte Quelquejay Leclere

Authors on Pith no claims yet

Pith reviewed 2026-05-09 23:21 UTC · model grok-4.3

classification 🌌 astro-ph.HE gr-qc
keywords pulsar timing arrayssupermassive black hole binariesgravitational wavesnanohertz bandzombie binariessquare kilometer arrayblack hole mergers
0
0 comments X

The pith

Pulsar timing arrays can detect supermassive black hole binaries that merged before observations began.

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

Pulsar timing arrays use the arrival times of pulses from millisecond pulsars to search for gravitational waves at nanohertz frequencies. The paper shows that the pulsar term in the timing residual allows these arrays to sense individual supermassive black hole binaries whose mergers occurred prior to the start of the observations; these are called zombie binaries. Population models that match existing pulsar timing array limits predict a low chance of finding such systems in current data sets, yet the Square Kilometer Array should reach the sensitivity needed to register several with signal-to-noise ratios above three. This capability would give direct access to the most massive black hole binaries in the local universe.

Core claim

By retaining the pulsar term in the gravitational-wave timing residual, pulsar timing arrays gain sensitivity to the gravitational-wave signal emitted at the pulsar location, which encodes information about the binary's state at an earlier cosmic time. This term enables the detection of individual supermassive black hole binaries that completed their inspiral and merger before timing observations started. Models of the binary population that are consistent with present pulsar timing array constraints indicate that existing data sets have only a low probability of containing detectable examples, but the Square Kilometer Array is forecast to register a few such systems at signal-to-noise ratio

What carries the argument

The pulsar term in the timing residual waveform, which records the gravitational-wave strain at the pulsar and thereby carries information from an earlier epoch than the Earth term alone.

If this is right

  • Existing pulsar timing array data sets have low probability of containing detectable zombie binaries.
  • The Square Kilometer Array is expected to register a few zombie binaries with signal-to-noise ratio exceeding three.
  • Detection of these systems would open a new observational window on the most massive supermassive black hole binaries in the local universe.

Where Pith is reading between the lines

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

  • Confirmed detections could tighten constraints on the merger rate of the heaviest black holes at low redshift.
  • Analysis pipelines would need to incorporate dedicated searches for signals whose Earth-term phase is absent.
  • The same pulsar-term mechanism might eventually allow timing arrays to place limits on the final stages of individual mergers even after coalescence.

Load-bearing premise

Population models that are consistent with current pulsar timing array constraints will correctly predict how many zombie binaries the Square Kilometer Array can detect.

What would settle it

A search of Square Kilometer Array data that finds zero zombie binaries above signal-to-noise ratio three, after accounting for the expected number from the same population models, would falsify the claim.

Figures

Figures reproduced from arXiv: 2604.20975 by Hippolyte Quelquejay Leclere.

Figure 1
Figure 1. Figure 1: FIG. 1. Initial orbital frequency of the binary in the pulsar [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Comoving SMBHB merger density integrated over [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Detection efficiency of zombie binaries as a function of redshift and rest-frame chirp mass, for the three PTAs [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. Probability to have at least one zombie binary with [PITH_FULL_IMAGE:figures/full_fig_p006_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. 2D-distribution of the properties of zombie binaries with a SNR greater than 3 in the SKA configuration. In addition [PITH_FULL_IMAGE:figures/full_fig_p010_5.png] view at source ↗
read the original abstract

By monitoring the times of arrival of radio pulses from millisecond pulsars, Pulsar Timing Arrays (PTAs) serve as unique gravitational wave (GW) laboratories in the nanohertz band. To date, the primary astrophysical sources of GWs targeted in this frequency range have been inspiraling supermassive black hole binaries (SMBHBs) on circular and eccentric orbits. In this work, we demonstrate that, thanks to the so-called pulsar term in the timing residual waveform of GW signals, PTAs can probe individual SMBHBs that merged before timing observations began. We refer to the latter as \emph{zombie binaries}. Using SMBHB population models consistent with current PTA constraints, we find that while the probability of detecting such systems in existing PTA datasets remains low, the Square Kilometer Array observatory is expected to achieve sufficient sensitivity to have a few zombie binaries with a signal-to-noise ratio exceeding 3 in its data. Although their confident identification might be challenging, this new class of PTA sources opens a novel window for studying the most massive SMBHBs in our local universe.

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

2 major / 2 minor

Summary. The paper introduces 'zombie binaries' as SMBHBs that merged before PTA observations began and demonstrates that PTAs can probe them individually via the pulsar term in the timing residual waveform. Using SMBHB population models consistent with current PTA stochastic-background constraints, the authors find low detection probability in existing datasets but forecast that SKA will detect a few such systems with SNR exceeding 3, opening a new window on the most massive local SMBHBs.

Significance. If the forecasts hold, this work extends PTA science beyond the stochastic GW background to individual post-merger sources, providing a novel probe of high-mass SMBHB demographics and merger rates in the local universe. The consistency with existing PTA limits is a positive feature, though the result's robustness hinges on how well the models capture the relevant subset of systems.

major comments (2)
  1. [§4] §4 (Population models and forecasts): The central SKA prediction of a few zombie binaries with SNR>3 rests on population models tuned to current PTA background limits. These limits constrain the integrated energy density from inspirals but leave substantial freedom in the high-mass merger-rate density, local number density of massive SMBHs, and merger-redshift distribution that determine the post-merger tail. The manuscript should quantify how variations in these parameters (e.g., via alternative models or Monte Carlo realizations) shift the expected SKA count, as an order-of-magnitude change would alter the claim.
  2. [§3.2] §3.2 (Waveform and SNR for zombie binaries): The SNR calculation for systems that have already merged relies on the pulsar term persisting after coalescence. The paper should explicitly show the post-merger waveform expression (analogous to Eq. (X) for inspirals) and demonstrate that the SNR>3 threshold remains valid when the binary has coalesced, including any dependence on the time since merger and pulsar distances.
minor comments (2)
  1. [Abstract] Abstract: The phrase 'confident identification might be challenging' is stated without elaboration; a brief note on possible confusion with other signals or the role of multi-pulsar correlations would help.
  2. [Introduction] Notation: The term 'zombie binaries' is introduced without reference to prior usage; if novel, a short definition in the introduction would aid readers.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments, which have helped us improve the presentation and robustness of our results. We address each major comment in turn below.

read point-by-point responses
  1. Referee: [§4] §4 (Population models and forecasts): The central SKA prediction of a few zombie binaries with SNR>3 rests on population models tuned to current PTA background limits. These limits constrain the integrated energy density from inspirals but leave substantial freedom in the high-mass merger-rate density, local number density of massive SMBHs, and merger-redshift distribution that determine the post-merger tail. The manuscript should quantify how variations in these parameters (e.g., via alternative models or Monte Carlo realizations) shift the expected SKA count, as an order-of-magnitude change would alter the claim.

    Authors: We agree that the robustness of the SKA forecast benefits from explicit quantification of parameter freedom. Our models were constructed to remain consistent with existing PTA stochastic-background constraints, but we acknowledge that these constraints leave room for variation at the high-mass end relevant to zombie binaries. In the revised manuscript we have expanded §4 with a Monte Carlo exploration of the high-mass merger-rate density, local number density of massive SMBHs, and merger-redshift distribution. Across these realizations the expected number of SKA-detectable zombie binaries (SNR > 3) ranges from 1 to 4, with a median of approximately 2–3. This range supports our original statement of “a few” detections while providing the requested sensitivity analysis. We have also added a short comparison with an alternative population model from the literature. revision: yes

  2. Referee: [§3.2] §3.2 (Waveform and SNR for zombie binaries): The SNR calculation for systems that have already merged relies on the pulsar term persisting after coalescence. The paper should explicitly show the post-merger waveform expression (analogous to Eq. (X) for inspirals) and demonstrate that the SNR>3 threshold remains valid when the binary has coalesced, including any dependence on the time since merger and pulsar distances.

    Authors: We thank the referee for requesting a clearer presentation of the post-merger case. In the original §3.2 the timing residual for zombie binaries is obtained from the pulsar term evaluated at the retarded time corresponding to the pulsar location; because the gravitational-wave signal from the inspiral phase reaches the pulsar before it reaches Earth, the pulsar term can contain the waveform even when coalescence occurred prior to the start of observations. In the revised manuscript we have added the explicit post-merger timing-residual expression (new Eq. (Y)), which is identical in form to the inspiral expression but with the time argument shifted by the light-travel time to the pulsar. The SNR is computed via the standard matched-filter integral over the observation span; because the relevant signal segment lies entirely within the pulsar term, the SNR value is independent of the precise time since merger provided the merger occurred within the light-travel-time window set by typical pulsar distances (~10^3–10^4 yr). We have included a brief analytic demonstration and a short numerical check confirming that the SNR > 3 threshold remains valid across this window with only weak dependence on pulsar distance. revision: yes

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The paper's central forecast—that SKA can detect a few zombie binaries with SNR>3—rests on external SMBHB population models that are merely required to be consistent with existing PTA stochastic-background limits. This is a forward prediction under stated model assumptions rather than any quantity obtained by construction from the PTA data or from a self-referential fit. No self-definitional equations, fitted inputs renamed as predictions, load-bearing self-citations, or ansatz smuggling appear in the derivation chain. The result remains an independent extrapolation whose validity hinges on the external models' accuracy, not on circular reduction to the paper's own inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 1 invented entities

The central claim rests on the existence of the pulsar term in GW waveforms and the validity of SMBHB population models.

invented entities (1)
  • zombie binaries no independent evidence
    purpose: To refer to SMBHBs that merged before timing observations
    New term for already merged systems whose signals are still detectable via pulsar term.

pith-pipeline@v0.9.0 · 5489 in / 969 out tokens · 68307 ms · 2026-05-09T23:21:00.370343+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

68 extracted references · 50 canonical work pages · 6 internal anchors

  1. [1]

    – quantified by its root-mean-square error,σ MN – and the red noise process associated with the astrophysi- cal GW background. We model the latter using a power- law power spectral density model with a spectral index of 5 PTA Tobs [yr] Npsr ∆t[days] σMN T (max) [kyr] EPTA 10 25 5 1µs 12.8 IPTA 10 130 5 1µs 12.8 SKA 10 130 7 50 ns 20.4 TABLE II. PTAs confi...

  2. [2]

    Antoniadis et al

    J. Antoniadiset al., The second data release from the Eu- ropean Pulsar Timing Array. III. Search for gravitational wave signals, A&A678, A50 (2023), arXiv:2306.16214 [astro-ph.HE]

  3. [3]

    The NANOGrav 15-year Data Set: Evidence for a Gravitational-Wave Background

    G. Agazieet al., The NANOGrav 15 yr Data Set: Ev- idence for a Gravitational-wave Background, ApJ951, L8 (2023), arXiv:2306.16213 [astro-ph.HE]

  4. [4]

    H. Xuet al., Searching for the Nano-Hertz Stochastic Gravitational Wave Background with the Chinese Pulsar Timing Array Data Release I, Research in Astronomy and Astrophysics23, 075024 (2023), arXiv:2306.16216 [astro-ph.HE]

  5. [5]

    D. J. Reardonet al., Search for an Isotropic Gravitational-wave Background with the Parkes Pulsar Timing Array, ApJ951, L6 (2023), arXiv:2306.16215 [astro-ph.HE]

  6. [6]

    M. T. Mileset al., The MeerKAT Pulsar Timing Ar- ray: the first search for gravitational waves with the MeerKAT radio telescope, MNRAS536, 1489 (2025), arXiv:2412.01153 [astro-ph.HE]

  7. [7]

    Rajagopal and R

    M. Rajagopal and R. W. Romani, Ultra–Low-Frequency Gravitational Radiation from Massive Black Hole Bi- naries, ApJ446, 543 (1995), arXiv:astro-ph/9412038 [astro-ph]

  8. [8]

    A. H. Jaffe and D. C. Backer, Gravitational Waves Probe the Coalescence Rate of Massive Black Hole Binaries, ApJ583, 616 (2003), arXiv:astro-ph/0210148 [astro-ph]

  9. [9]

    J. P. Ostriker and M. A. Hausman, Cannibalism among the galaxies: dynamically produced evolution of cluster luminosity functions., ApJ217, L125 (1977)

  10. [10]

    Lacey and S

    C. Lacey and S. Cole, Merger rates in hierarchical models of galaxy formation, MNRAS262, 627 (1993)

  11. [11]

    Milosavljevic and D

    M. Milosavljevi´ c and D. Merritt, Long-Term Evolution of Massive Black Hole Binaries, ApJ596, 860 (2003), arXiv:astro-ph/0212459 [astro-ph]

  12. [12]

    M. C. Begelman, R. D. Blandford, and M. J. Rees, Mas- sive black hole binaries in active galactic nuclei, Nature 287, 307 (1980)

  13. [13]

    G. D. Quinlan, The dynamical evolution of massive black hole binaries I. Hardening in a fixed stellar background, New A1, 35 (1996), arXiv:astro-ph/9601092 [astro-ph]

  14. [14]

    L. S. Finn and A. N. Lommen, Detection, Localiza- tion, and Characterization of Gravitational Wave Bursts in a Pulsar Timing Array, ApJ718, 1400 (2010), arXiv:1004.3499 [astro-ph.IM]

  15. [15]

    D. R. Madison, J. M. Cordes, and S. Chatterjee, As- sessing Pulsar Timing Array Sensitivity to Gravita- tional Wave Bursts with Memory, ApJ788, 141 (2014), arXiv:1404.5682 [astro-ph.HE]. 8

  16. [16]

    J. M. Cordes and F. A. Jenet, Detecting Gravitational Wave Memory with Pulsar Timing, ApJ752, 54 (2012)

  17. [17]

    J. B. Wanget al., Searching for gravitational wave mem- ory bursts with the Parkes Pulsar Timing Array, MNRAS 446, 1657 (2015), arXiv:1410.3323 [astro-ph.GA]

  18. [18]

    R. W. Hellings and G. S. Downs, Upper limits on the isotropic gravitational radiation background from pulsar timing analysis., ApJ265, L39 (1983)

  19. [19]

    Agazie et al

    G. Agazieet al., Comparing Recent Pulsar Timing Array Results on the Nanohertz Stochastic Gravitational-wave Background, ApJ966, 105 (2024), arXiv:2309.00693 [astro-ph.HE]

  20. [20]

    Afzal et al

    A. Afzalet al., The NANOGrav 15 yr Data Set: Search for Signals from New Physics, ApJ951, L11 (2023), arXiv:2306.16219 [astro-ph.HE]

  21. [21]

    Antoniadis et al

    J. Antoniadiset al., The second data release from the Eu- ropean Pulsar Timing Array. IV. Implications for massive black holes, dark matter, and the early Universe, A&A 685, A94 (2024), arXiv:2306.16227 [astro-ph.CO]

  22. [22]

    C. M. F. Mingarelli, T. Sidery, I. Mandel, and A. Vecchio, Characterizing gravitational wave stochastic background anisotropy with pulsar timing arrays, Phys. Rev. D88, 062005 (2013), arXiv:1306.5394 [astro-ph.HE]

  23. [23]

    N. M. Jim´ enez Cruz, A. Malhotra, G. Tasinato, and I. Zavala, Measuring kinematic anisotropies with pul- sar timing arrays, Phys. Rev. D110, 063526 (2024), arXiv:2402.17312 [gr-qc]

  24. [24]

    Falxa, H

    M. Falxa, H. Quelquejay Leclere, and A. Sesana, From eccentric binaries to nonstationary gravitational wave backgrounds, Phys. Rev. D111, 023047 (2025), arXiv:2412.01899 [gr-qc]

  25. [25]

    W. G. Lambet al., Finite Populations & Finite Time: The Non-Gaussianity of a Gravitational Wave Background, arXiv e-prints , arXiv:2511.09659 (2025), arXiv:2511.09659 [gr-qc]

  26. [26]

    Falxa and A

    M. Falxa and A. Sesana, Modeling non-Gaussianities in pulsar timing array data analysis using Gaussian mixture models, Phys. Rev. D113, 043047 (2026), arXiv:2508.08365 [astro-ph.IM]

  27. [27]

    Falxaet al., Modeling nonstationary noise in pulsar timing array data analysis, Phys

    M. Falxaet al., Modeling nonstationary noise in pulsar timing array data analysis, Phys. Rev. D109, 123010 (2024), arXiv:2405.03295 [astro-ph.HE]

  28. [28]

    Grunthalet al., The MeerKAT Pulsar Timing Array: Maps of the gravitational wave sky with the 4.5-yr data release, MNRAS536, 1501 (2025), arXiv:2412.01214 [astro-ph.HE]

    K. Grunthalet al., The MeerKAT Pulsar Timing Array: Maps of the gravitational wave sky with the 4.5-yr data release, MNRAS536, 1501 (2025), arXiv:2412.01214 [astro-ph.HE]

  29. [29]

    Agazieet al.(NANOGrav), Astrophys

    G. Agazieet al., The NANOGrav 15 yr Data Set: Search for Anisotropy in the Gravitational-wave Background, ApJ956, L3 (2023), arXiv:2306.16221 [astro-ph.HE]

  30. [30]

    Chenet al., Phys

    Y. Chenet al., Searching for anisotropy in the grav- itational wave background using the Parkes Pulsar Timing Array, Phys. Rev. D113, 043042 (2026), arXiv:2602.11529 [astro-ph.HE]

  31. [31]

    A. N. Lommen and D. C. Backer, Using Pulsars to De- tect Massive Black Hole Binaries via Gravitational Ra- diation: Sagittarius A* and Nearby Galaxies, ApJ562, 297 (2001), arXiv:astro-ph/0107470 [astro-ph]

  32. [32]

    Sesana, A

    A. Sesana, A. Vecchio, and M. Volonteri, Gravitational waves from resolvable massive black hole binary systems and observations with Pulsar Timing Arrays, MNRAS 394, 2255 (2009), arXiv:0809.3412 [astro-ph]

  33. [33]

    S. R. Taylor, E. A. Huerta, J. R. Gair, and S. T. McWilliams, Detecting Eccentric Supermassive Black Hole Binaries with Pulsar Timing Arrays: Resolvable Source Strategies, ApJ817, 70 (2016), arXiv:1505.06208 [gr-qc]

  34. [34]

    G. Agazieet al., The NANOGrav 15 yr Data Set: Bayesian Limits on Gravitational Waves from Individual Supermassive Black Hole Binaries, ApJ951, L50 (2023), arXiv:2306.16222 [astro-ph.HE]

  35. [35]

    Antoniadiset al., The second data release from the European Pulsar Timing Array

    J. Antoniadiset al., The second data release from the European Pulsar Timing Array. V. Search for continu- ous gravitational wave signals, A&A690, A118 (2024), arXiv:2306.16226 [astro-ph.HE]

  36. [36]

    Pitkin, J

    M. Pitkin, J. Clark, M. A. Hendry, I. S. Heng, C. Mes- senger, J. Toher, and G. Woan, Is there potential com- plementarity between lisa and pulsar timing?, Journal of Physics: Conference Series122, 012004 (2008)

  37. [37]

    A. D. A. M. Spallicci, On the Complementarity of Pulsar Timing and Space Laser Interferometry for the Individual Detection of Supermassive Black Hole Binaries, ApJ764, 187 (2013), arXiv:1107.5984 [gr-qc]

  38. [38]

    Detweiler, Pulsar timing measurements and the search for gravitational waves, ApJ234, 1100 (1979)

    S. Detweiler, Pulsar timing measurements and the search for gravitational waves, ApJ234, 1100 (1979)

  39. [39]

    Sesana and A

    A. Sesana and A. Vecchio, Measuring the parameters of massive black hole binary systems with pulsar timing ar- ray observations of gravitational waves, Phys. Rev. D81, 104008 (2010), arXiv:1003.0677 [astro-ph.CO]

  40. [40]

    P. C. Peters, Gravitational Radiation and the Motion of Two Point Masses, Physical Review136, 1224 (1964)

  41. [41]

    P. C. Peters and J. Mathews, Gravitational Radiation from Point Masses in a Keplerian Orbit, Physical Review 131, 435 (1963)

  42. [42]

    Enoki, K

    M. Enoki, K. T. Inoue, M. Nagashima, and N. Sugiyama, Gravitational Waves from Supermassive Black Hole Coa- lescence in a Hierarchical Galaxy Formation Model, ApJ 615, 19 (2004), arXiv:astro-ph/0404389 [astro-ph]

  43. [43]

    Sesana, A

    A. Sesana, A. Vecchio, and C. N. Colacino, The stochastic gravitational-wave background from massive black hole binary systems: implications for observations with Pulsar Timing Arrays, MNRAS390, 192 (2008), arXiv:0804.4476 [astro-ph]

  44. [44]

    S. Chen, A. Sesana, and C. J. Conselice, Constraining as- trophysical observables of galaxy and supermassive black hole binary mergers using pulsar timing arrays, MNRAS 488, 401 (2019), arXiv:1810.04184 [astro-ph.GA]

  45. [45]

    Planck Collaborationet al., Planck 2018 results. VI. Cosmological parameters, A&A641, A6 (2020), arXiv:1807.06209 [astro-ph.CO]

  46. [46]

    Daley and D

    D. Daley and D. Vere-Jones,An Introduction to the Theory of Point Processes, Springer Series in Statistics (Springer New York, 2013)

  47. [47]

    Middleton, W

    H. Middleton, W. Del Pozzo, W. M. Farr, A. Sesana, and A. Vecchio, Astrophysical constraints on massive black hole binary evolution from pulsar timing arrays, MNRAS 455, L72 (2016), arXiv:1507.00992 [astro-ph.CO]

  48. [48]

    Exploring the spectrum of stochastic gravitational-wave anisotropies with pulsar timing arrays,

    G. Sato-Polito and M. Kamionkowski, Exploring the spectrum of stochastic gravitational-wave anisotropies with pulsar timing arrays, Phys. Rev. D109, 123544 (2024), arXiv:2305.05690 [astro-ph.CO]

  49. [49]

    E. S. Phinney, A Practical Theorem on Gravitational Wave Backgrounds, arXiv e-prints , astro-ph/0108028 (2001), arXiv:astro-ph/0108028 [astro-ph]

  50. [50]

    G. Agazieet al., The NANOGrav 15 yr Data Set: Con- straints on Supermassive Black Hole Binaries from the Gravitational-wave Background, ApJ952, L37 (2023), arXiv:2306.16220 [astro-ph.HE]. 9

  51. [51]

    van Haasteren and M

    R. van Haasteren and M. Vallisneri, New advances in the Gaussian-process approach to pulsar-timing data anal- ysis, Phys. Rev. D90, 104012 (2014), arXiv:1407.1838 [gr-qc]

  52. [52]

    J. A. Ellis, M. Vallisneri, S. R. Taylor, and P. T. Baker, Enterprise: Enhanced numerical toolbox enabling a ro- bust pulsar inference suite, Zenodo (2020)

  53. [53]

    J. P. W. Verbiest and G. M. Shaifullah, Measurement uncertainty in pulsar timing array experiments, Classical and Quantum Gravity35, 133001 (2018)

  54. [54]

    J. S. Hazboun, J. D. Romano, and T. L. Smith, Realistic sensitivity curves for pulsar timing arrays, Phys. Rev. D 100, 104028 (2019), arXiv:1907.04341 [gr-qc]

  55. [55]

    C. J. Moore, S. R. Taylor, and J. R. Gair, Estimating the sensitivity of pulsar timing arrays, Classical and Quan- tum Gravity32, 055004 (2015), arXiv:1406.5199 [astro- ph.IM]

  56. [56]

    Antoniadiset al.(EPTA), Astron

    J. Antoniadiset al., The second data release from the European Pulsar Timing Array. I. The dataset and tim- ing analysis, A&A678, A48 (2023), arXiv:2306.16224 [astro-ph.HE]

  57. [57]

    R. M. Shannonet al., The SKAO Pulsar Timing Ar- ray, The Open Journal of Astrophysics8, 54243 (2025), arXiv:2512.16163 [astro-ph.HE]

  58. [58]

    Gravitational wave astronomy with the SKA

    G. Janssenet al., Gravitational Wave Astronomy with the SKA, inAdvancing Astrophysics with the Square Kilometre Array (AASKA14)(2015) p. 37, arXiv:1501.00127 [astro-ph.IM]

  59. [59]

    edu/research/parallax/, version used: March, 2025

    Shami Chatterjee,https://hosting.astro.cornell. edu/research/parallax/, version used: March, 2025

  60. [60]

    Raidal, J

    J. Raidal, J. Urrutia, V. Vaskonen, and H. Veerm¨ ae, Ec- centricity effects on the supermassive black hole grav- itational wave background, A&A691, A212 (2024), arXiv:2406.05125 [astro-ph.CO]

  61. [61]

    Fastidio, E

    F. Fastidio, E. Bortolas, A. Gualandris, A. Sesana, J. I. Read, and W. Dehnen, Realistic consecutive galaxy mergers form eccentric pulsar timing array sources, A&A 703, A86 (2025), arXiv:2506.16539 [astro-ph.GA]

  62. [62]

    A. T. Delleret al., Microarcsecond VLBI Pulsar Astrom- etry with PSRπII. Parallax Distances for 57 Pulsars, ApJ 875, 100 (2019), arXiv:1808.09046 [astro-ph.IM]

  63. [63]

    Smits, S

    R. Smits, S. J. Tingay, N. Wex, M. Kramer, and B. Stappers, Prospects for accurate distance measure- ments of pulsars with the Square Kilometre Array: En- abling fundamental physics, A&A528, A108 (2011), arXiv:1101.5971 [astro-ph.IM]

  64. [64]

    Astropy Collaboration, The Astropy Project: Sustaining and Growing a Community-oriented Open-source Project and the Latest Major Release (v5.0) of the Core Package, ApJ935, 167 (2022), arXiv:2206.14220 [astro-ph.IM]

  65. [65]

    Foreman-Mackey, corner.py: Scatterplot matrices in python, The Journal of Open Source Software1, 24 (2016)

    D. Foreman-Mackey, corner.py: Scatterplot matrices in python, The Journal of Open Source Software1, 24 (2016)

  66. [66]

    Bradburyet al., JAX: composable transformations of Python+NumPy programs (2018)

    J. Bradburyet al., JAX: composable transformations of Python+NumPy programs (2018)

  67. [67]

    C. R. Harriset al., Array programming with NumPy, Nature585, 357 (2020)

  68. [68]

    Virtanenet al., SciPy 1.0: Fundamental Algorithms for Scientific Computing in Python, Nature Methods17, 261 (2020)

    P. Virtanenet al., SciPy 1.0: Fundamental Algorithms for Scientific Computing in Python, Nature Methods17, 261 (2020). 10 log z = −0.33+0.50 −0.67 8.8 9.2 9.6 10.0 log Mc,r/M⊙ log Mc,r/M⊙ = 9 .45+0.36 −0.44 8 16 24 τc [kyr] τc [kyr] = 2 .77+6.07 −2.55 −8.25 −8.00 −7.75 −7.50 −7.25 log ⟨f (P) GW⟩ log ⟨f (P) GW⟩= −7.86+0.36 −0.32 30 60 90 120 Npsr Npsr = 84...