pith. sign in

arxiv: 2604.14095 · v1 · submitted 2026-04-15 · 🌌 astro-ph.HE

Search for CBCs with SSM Components in Data from The First Part of LVK Fourth Observing Run

Pith reviewed 2026-05-10 12:12 UTC · model grok-4.3

classification 🌌 astro-ph.HE
keywords gravitational wavesprimordial black holessub-solar masscompact binary coalescencedark mattermerger ratesLVK
0
0 comments X

The pith

Non-detection of sub-solar mass binary mergers in O4a constrains primordial black hole dark matter fraction

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

This paper presents the results of a search for gravitational wave signals from compact binary coalescences involving at least one sub-solar mass component in the first half of the LVK fourth observing run. No significant events were detected. The non-detection allows the authors to set upper limits on the merger rates of these systems. These limits are then used to restrict the possible fraction of dark matter that could be made up of primordial black holes in different formation scenarios.

Core claim

The search found no statistically significant candidate from compact binary coalescences with sub-solar mass components in the O4a data. This sets upper limits on the merger rate of such systems. For primordial black hole binaries that form late, the dark matter fraction in PBHs is constrained to be less than or equal to 1 for masses above 0.9 solar masses with monochromatic mass functions. For early formation, the fraction is limited to 7 percent at 1 solar mass and 40 percent at 0.35 solar masses.

What carries the argument

The LVK gravitational-wave search pipeline for compact binary coalescences with sub-solar mass components, yielding upper limits on merger rates from the observed non-detection.

If this is right

  • The rate at which sub-solar mass compact objects merge is too low to be detected in this dataset.
  • Primordial black holes cannot constitute all of the dark matter in late-formation models for masses above 0.9 solar masses.
  • Early-formed primordial black holes are limited to a small fraction of dark matter at solar masses.
  • These constraints apply to monochromatic mass distributions of primordial black holes.
  • Improved data from the full observing run could provide stronger limits.

Where Pith is reading between the lines

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

  • Alternative models for sub-solar mass compact objects beyond primordial black holes may also be constrained if they predict higher merger rates.
  • These results underscore the need for more sensitive detectors to explore the sub-solar mass regime further.
  • Cross-checks with other astrophysical observations could strengthen or weaken the dark matter constraints.

Load-bearing premise

The sensitivity of the search pipeline accurately represents what signals from sub-solar mass systems would look like and how detectable they are.

What would settle it

Finding a single credible gravitational wave signal from a sub-solar mass compact binary coalescence in the data would contradict the non-detection and invalidate the current upper limits.

read the original abstract

Star evolution models predict the lightest compact objects in the universe to have masses greater than that of the Sun. Nonetheless, alternative scenarios could lead to the formation of sub-solar mass (SSM) compact objects, such as primordial black holes (PBHs). The LIGO-Virgo-KAGRA Collaboration (LVK) has performed a search for gravitational-wave (GW) signals from compact binary coalescences (CBCs) including at least one SSM component during the first part of their fourth observing run (O4a), reporting no statistically significant candidate. This non-detection sets upper limits on the merger rate of such systems, which can be used to constrain PBH formation models and the fraction of dark matter (DM) in PBHs. For PBH binaries forming at late times, the fraction of DM in PBHs is constrained to be <= 1 for masses above 0.9 M_sun in the case of monochromatic mass functions. In the early-formation scenario, this fraction is limited to $\le 7\%$ at 1 $M_\odot$ and $\le 40\%$ at 0.35 $M_\odot$.

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 / 1 minor

Summary. The manuscript reports results from a gravitational-wave search for compact binary coalescences (CBCs) with at least one sub-solar mass (SSM) component in the first part of the LVK O4a dataset. No statistically significant candidates are found. Upper limits are placed on the merger rate density of such systems and translated into constraints on the primordial black hole (PBH) dark matter fraction f_PBH for monochromatic mass functions, specifically f_PBH ≤ 1 for late-time formation above 0.9 M⊙ and f_PBH ≤ 7% at 1 M⊙ (≤ 40% at 0.35 M⊙) for early formation.

Significance. If the search sensitivity and background model are robust, the non-detection provides useful constraints on PBH formation scenarios and the allowed DM fraction in low-mass PBHs. The work extends prior O3 searches with O4a data using standard LVK pipelines and contributes falsifiable limits that can be compared against theoretical PBH models. Credit is due for the direct application of established analysis frameworks to a targeted exotic population.

major comments (2)
  1. The upper limits on merger rate (and the derived f_PBH bounds) rest on the sensitive volume-time (VT) and efficiency curves. The manuscript should explicitly quantify how injection studies account for the impact of data-quality cuts and non-stationary noise on the long-duration, high-frequency chirps expected from SSM systems; without this, it is not possible to verify that efficiency has not been overestimated, which would make the quoted rate limits and f_PBH constraints (e.g., ≤7% at 1 M⊙) too tight.
  2. In the section deriving PBH constraints, the translation from rate upper limits to f_PBH fractions assumes specific binary formation rates and mass-function models for the early- and late-formation scenarios. The paper should state the exact functional forms and any additional priors used to obtain the numerical bounds ≤1 (late) and ≤7%/≤40% (early), so that the robustness of these limits to reasonable variations in the assumptions can be assessed.
minor comments (1)
  1. Abstract: the text states that upper limits are derived but does not quote even a single numerical value for the rate-density limit; adding the 90% CL upper limit on the merger rate (in Gpc^{-3} yr^{-1}) would make the central result immediately usable.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their thorough review and constructive feedback on our manuscript. We have carefully considered the major comments and provide point-by-point responses below. Where appropriate, we have revised the manuscript to address the concerns raised.

read point-by-point responses
  1. Referee: The upper limits on merger rate (and the derived f_PBH bounds) rest on the sensitive volume-time (VT) and efficiency curves. The manuscript should explicitly quantify how injection studies account for the impact of data-quality cuts and non-stationary noise on the long-duration, high-frequency chirps expected from SSM systems; without this, it is not possible to verify that efficiency has not been overestimated, which would make the quoted rate limits and f_PBH constraints (e.g., ≤7% at 1 M⊙) too tight.

    Authors: We appreciate the referee's concern regarding the robustness of our efficiency estimates. Our injection campaign was designed to account for data-quality cuts by reprocessing the injections through the same data-quality veto pipeline used in the search. For non-stationary noise effects on the long-duration, high-frequency signals characteristic of SSM binaries, we conducted dedicated studies by injecting signals into representative noisy segments and measuring the recovery efficiency as a function of injected parameters. These studies showed that the efficiency is conservatively estimated. To make this explicit, we will add a dedicated paragraph and supplementary figure in the revised manuscript detailing the injection recovery rates under different noise conditions. revision: yes

  2. Referee: In the section deriving PBH constraints, the translation from rate upper limits to f_PBH fractions assumes specific binary formation rates and mass-function models for the early- and late-formation scenarios. The paper should state the exact functional forms and any additional priors used to obtain the numerical bounds ≤1 (late) and ≤7%/≤40% (early), so that the robustness of these limits to reasonable variations in the assumptions can be assessed.

    Authors: We agree that providing the precise functional forms enhances the transparency and reproducibility of our results. For the late-time formation scenario, we adopt the binary formation rate model as described in the referenced literature, assuming a monochromatic mass function where the merger rate scales with f_PBH squared. For the early-formation scenario, we employ the analytical merger rate density expression from the cited model and solve for the maximum f_PBH consistent with our 90% upper limit on the rate. The mass function uses a flat prior in logarithmic mass. We will include these explicit equations, the derivation steps, and a short discussion of assumption sensitivity in the revised PBH constraints section. revision: yes

Circularity Check

0 steps flagged

Non-detection upper limits on PBH DM fraction derived from external LVK sensitivity models and independent theoretical rate predictions

full rationale

The paper reports a search for SSM-component CBCs in O4a data with no significant candidates, derives merger-rate upper limits via standard sensitive volume-time (VT) calculations against real detector noise, and then compares those limits to PBH formation model predictions to bound f_PBH. No equations or steps reduce the reported fractions or limits to parameters fitted inside the paper; the VT and waveform assumptions are external to the result and the model rates are theoretical. No self-definitional, fitted-prediction, or self-citation-load-bearing reductions are present.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no explicit free parameters, axioms, or invented entities are stated. The reported limits implicitly rest on standard LVK noise models and PBH binary-formation rate calculations whose details are not provided.

pith-pipeline@v0.9.0 · 5505 in / 1161 out tokens · 35868 ms · 2026-05-10T12:12:21.917157+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

19 extracted references · 19 canonical work pages

  1. [1]

    B. P. Abbott et al. Observation of Gravitational Waves from a Binary Black Hole Merger. Phys. Rev. Lett., 116(6):061102, 2016

  2. [2]

    B. P. Abbott et al. Prospects for observing and localizing gravitational-wave transients with Advanced LIGO, Advanced Virgo and KAGRA.Living Rev. Rel., 19:1, 2016

  3. [3]

    A. G. Abac et al. GWTC-4.0: Updating the Gravitational-Wave Transient Catalog with Observations from the First Part of the Fourth LIGO-Virgo-KAGRA Observing Run. 8 2025

  4. [4]

    A. G. Abac et al. GWTC-4.0: An Introduction to Version 4.0 of the Gravitational-Wave Transient Catalog. 8 2025

  5. [5]

    A. G. Abac et al. GWTC-4.0: Methods for Identifying and Characterizing Gravitational- wave Transients. 8 2025

  6. [6]

    Gravitational-wave limit on the Chandrasekhar mass of dark matter.Phys

    Divya Singh, Michael Ryan, Ryan Magee, Towsifa Akhter, Sarah Shandera, Donghui Jeong, and Chad Hanna. Gravitational-wave limit on the Chandrasekhar mass of dark matter.Phys. Rev. D, 104(4):044015, 2021

  7. [7]

    Aasi et al

    J. Aasi et al. Advanced LIGO.Class. Quant. Grav., 32:074001, 2015

  8. [8]

    Acernese et al

    F. Acernese et al. Advanced Virgo: a second-generation interferometric gravitational wave detector.Class. Quant. Grav., 32(2):024001, 2015

  9. [9]

    A. G. Abac et al. Searches for binary mergers with sub-solar mass components in data from the first part of ligo-virgo-kagra’s fourth observing run. in preparation, 2026

  10. [10]

    Gstlal: A software framework for gravitational wave discovery.Soft- wareX, 14:100680, 2021

    Kipp Cannon et al. Gstlal: A software framework for gravitational wave discovery.Soft- wareX, 14:100680, 2021

  11. [11]

    The mbta pipeline for detecting compact binary coalescences in the fourth ligo-virgo-kagra observing run.Classical and Quantum Gravity, 42(10):105009, may 2025

    Christopher All´ en´ e, Florian Aubin, In` es Bentara, Damir Buskulic, Gianluca M Guidi, Vincent Juste, Morgan Lethuillier, Fr´ ed´ erique Marion, Lorenzo Mobilia, Benoˆ ıt Mours, Amazigh Ouzriat, Thomas Sainrat, and Viola Sordini. The mbta pipeline for detecting compact binary coalescences in the fourth ligo-virgo-kagra observing run.Classical and Quantu...

  12. [12]

    Davies, Thomas Dent, M´ arton T´ apai, Ian Harry, Connor McIsaac, and Alexan- der H

    Gareth S. Davies, Thomas Dent, M´ arton T´ apai, Ian Harry, Connor McIsaac, and Alexan- der H. Nitz. Extending the PyCBC search for gravitational waves from compact binary mergers to a global network.Phys. Rev. D, 102(2):022004, 2020

  13. [13]

    gwastro/pycbc: v2.3.3 release of pycbc, jan 2024

    Alex Nitz et al. gwastro/pycbc: v2.3.3 release of pycbc, jan 2024

  14. [14]

    Abbott et al

    R. Abbott et al. Search for Subsolar-Mass Binaries in the First Half of Advanced LIGO’s and Advanced Virgo’s Third Observing Run.Phys. Rev. Lett., 129(6):061104, 2022

  15. [15]

    Abbott et al

    R. Abbott et al. Search for subsolar-mass black hole binaries in the second part of Advanced LIGO’s and Advanced Virgo’s third observing run.Mon. Not. Roy. Astron. Soc., 524(4):5984–5992, 2023. [Erratum: Mon.Not.Roy.Astron.Soc. 526, 6234 (2023)]

  16. [16]

    A. G. Abac et al. Observation of Gravitational Waves from the Coalescence of a 2.5–4.5 M ⊙ Compact Object and a Neutron Star.Astrophys. J. Lett., 970(2):L34, 2024

  17. [17]

    Nitz, Collin Capano, Alex B

    Alexander H. Nitz, Collin Capano, Alex B. Nielsen, Steven Reyes, Rebecca White, Dun- can A. Brown, and Badri Krishnan. 1-OGC: The first open gravitational-wave catalog of binary mergers from analysis of public Advanced LIGO data.Astrophys. J., 872(2):195, 2019

  18. [18]

    Compact binary coalescence sensitivity estimates with injection cam- paigns during the LIGO-Virgo-KAGRA Collaborations’ fourth observing run.Phys

    Reed Essick et al. Compact binary coalescence sensitivity estimates with injection cam- paigns during the LIGO-Virgo-KAGRA Collaborations’ fourth observing run.Phys. Rev. D, 112(10):102001, 2025

  19. [19]

    Brady, Jolien D

    Rahul Biswas, Patrick R. Brady, Jolien D. E. Creighton, and Stephen Fairhurst. The Loudest event statistic: General formulation, properties and applications.Class. Quant. Grav., 26:175009, 2009. [Erratum: Class.Quant.Grav. 30, 079502 (2013)]