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arxiv: 2512.19077 · v2 · submitted 2025-12-22 · 🌀 gr-qc · astro-ph.CO· astro-ph.GA· astro-ph.HE

The First Model-Independent Upper Bound on Micro-lensing Signature of the Highest Mass Binary Black Hole Event GW231123

Pith reviewed 2026-05-16 20:54 UTC · model grok-4.3

classification 🌀 gr-qc astro-ph.COastro-ph.GAastro-ph.HE
keywords gravitational wavesmicrolensingbinary black holesGW231123gravitational lensingmodel-independent analysisO4a events
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The pith

No definitive microlensing detected in heaviest black hole merger GW231123, as waveform errors mask any signal

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

The paper examines the gravitational wave event GW231123, the most massive binary black hole merger recorded, to test whether gravitational lensing explains its unusually high inferred masses. Using a model-independent search method, it finds no conclusive lensing signature but notes a possible residual feature in the data that could match a microlensing modulation of amplitude up to 0.8 at 95 percent . The analysis shows that uncertainties in waveform modeling for heavy systems are large enough to hide true lensing effects in short signals like this one. This sets the first such upper bound and indicates that improved models will soon allow detection of similar lensed events if they exist.

Core claim

The mu-GLANCE analysis of GW231123 and other O4a events finds no strong evidence for microlensing. A residual feature appears consistent with a lensing modulation amplitude reaching 0.8 at 95 percent , yet waveform systematics in heavy binaries dominate short-duration signals and prevent any firm detection claim. If the event is lensed, comparable events should become identifiable with present detector sensitivity once waveform accuracy improves.

What carries the argument

mu-GLANCE, a model-independent method that cross-correlates residual strain across the detector network and performs Bayesian inference on possible lensing-induced modulations.

If this is right

  • If GW231123 is lensed, similar lensed events will become detectable with current detector sensitivity.
  • More accurate waveform models will open a new discovery channel for lensed gravitational waves.
  • This approach provides the first model-independent upper bound on microlensing for the highest-mass event.
  • Lensing remains a viable explanation for masses inside the pair-instability gap once systematics are controlled.

Where Pith is reading between the lines

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

  • Applying the same search to additional high-mass events could test whether lensing systematically inflates apparent masses.
  • Future runs with longer signals or better calibration may separate real modulations from modeling errors without relying on specific lens models.
  • Confirmation of microlensing would directly support alternative formation channels for black holes in the mass gap.

Load-bearing premise

Waveform modeling uncertainties for heavy binary black holes are large enough to completely hide or mimic any microlensing modulation in short signals.

What would settle it

A clear residual modulation persisting after waveform models for heavy binaries reduce their systematic errors below the 0.8 amplitude level.

Figures

Figures reproduced from arXiv: 2512.19077 by Aniruddha Chakraborty, Suvodip Mukherjee.

Figure 1
Figure 1. Figure 1: In this figure, we show the inference of GW source properties: detected BBH masses (m1 and m2), luminosity distance (dL), inclination angle (θjn), effective-spin (χeff ) and coalescence angle (ϕ). The results for five different waveform models are shown in different colors. The disagreement between the parameters recovered shows the high systematic uncertainties associated with the waveform modeling for hi… view at source ↗
Figure 2
Figure 2. Figure 2: In this figure, along the first column, we show the residuals in detector H1 and L1. In the second column, we show residual cross-correlation for two different timescales 1/8s and 1/16s, to show the variation of the residual cross-correlation with the associated timescale. In the third column we show cumulative residual cross-correlation. Each row is associated with the results given a waveform model, the … view at source ↗
Figure 3
Figure 3. Figure 3: In this figure, we show the estimation of the lensing parameters for different waveform models. The posteriors obtained for different waveform models agree on the values of the estimated lensing parameters. The estimations of the lensing parameters show consistency with the residual cross-correlation results: higher the residual cross-correlation SNR, higher the amplitude and phase distortions. appear due … view at source ↗
Figure 4
Figure 4. Figure 4: In this figure, we present our findings from the searches of wave-optics lensing features from the GWTC-4 catalog. The horizontal axis shows the events in chronological sequence, and the vertical axis shows the residual SNR. To keep waveform modeling errors in check, we considered only the portion of the waveform when the BBH orbit is larger than the innermost stable circular orbit (ISCO) the frequency of … view at source ↗
Figure 5
Figure 5. Figure 5: In the figure, we present the recovery of different GW source parameters by a set of waveform models for a simu￾lated heavy-mass (Mc = 80M⊙, q = 0.75) signal with IMRPhenomXPHM-SpinTaylor waveform with SNR similar to GW231123 (ρN = 22.78). The recovery has been performed with a set of three different waveform models: IMRPhenomTPHM, IMRPhenomXO4a and IMRPhenomXPHM-SpinTaylor. The quantity ρresidual captures… view at source ↗
Figure 6
Figure 6. Figure 6: In the figure, we present the recovery of different GW source parameters by a few different waveforms for a simulated heavy-mass (Mc = 100M⊙, q = 0.75) signal with IMRPhenomXPHM-SpinTaylor waveform with SNR similar to GW231123 (ρN = 22.77). The recovery has been performed with a set of three different waveform models: IMRPhenomTPHM, IMRPhenomXO4a and IMRPhenomXPHM-SpinTaylor. with a source chirp mass of 80… view at source ↗
Figure 7
Figure 7. Figure 7: In the figure, we present the recovery of different GW source parameters by a few different waveforms for a simulated heavy-mass (Mc = 120M⊙, q = 0.75) signal with IMRPhenomXPHM-SpinTaylor waveform with SNR similar to GW231123 (ρN = 22.80). The recovery has been performed with a set of three different waveform models: IMRPhenomTPHM, IMRPhenomXO4a and IMRPhenomXPHM-SpinTaylor [PITH_FULL_IMAGE:figures/full_… view at source ↗
read the original abstract

The recently discovered gravitational wave event, GW231123, is the most massive binary black hole merger detected to date. The inferred source masses of the event fall within the pair-instability supernova mass gap, where black holes formed directly from stellar progenitors are expected to be rare, making alternative formation scenarios for such massive black holes especially relevant. One proposed explanation is gravitational lensing, which can make the source masses to be inferred as higher than their true values. In this work, we search for lensing signatures in GW231123, together with other O4a events, using a model-independent approach with mu-GLANCE. The method tests residual strain for correlated features across the detector network via cross-correlation and infers lensing-induced modulations within a Bayesian framework. Our analysis finds no strong evidence for lensing in GW231123, but reveals a potential residual feature that could be consistent with microlensing, with a modulation amplitude of up to 0.8 at 95% confidence. However, we find that waveform systematics for such heavy binary systems are sufficiently large to shadow the lensing signatures in short-duration signals like GW231123, preventing any definitive claim of lensing at this stage. We conclude that, if this event is lensed, similar lensed events will be detectable in the near future with current detector sensitivity, opening a new discovery space for lensed gravitational waves with the aid of more accurate waveform models.

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 / 0 minor

Summary. The manuscript presents a model-independent search for microlensing signatures in the high-mass binary black hole event GW231123 (and other O4a events) using the mu-GLANCE framework. This involves cross-correlating residuals across the detector network and performing Bayesian inference on possible lensing-induced modulations. The analysis reports no strong evidence for lensing but identifies a potential residual feature consistent with microlensing, with a modulation amplitude upper bound of 0.8 at 95% confidence. The authors conclude that waveform systematics for heavy BBH systems are large enough to shadow such signatures in short-duration signals, preventing a definitive lensing claim, while noting that improved waveform models could enable future detections.

Significance. If the central claim holds after addressing the quantitative gap in systematics, the work would deliver the first model-independent upper bound on microlensing for the highest-mass GW event and demonstrate the utility of residual cross-correlation methods for lensing searches. It highlights a key limitation in current waveform accuracy for pair-instability-gap masses and provides a concrete path for future O4/O5 analyses to test lensing hypotheses without relying on specific lens models.

major comments (1)
  1. [Abstract and results section on waveform systematics] The claim that waveform systematics for heavy binary systems are sufficiently large to shadow the lensing signatures (abstract and results/discussion) is load-bearing for the decision to withhold a definitive lensing statement, yet it is supported only qualitatively. No direct error budget or comparison is shown between the observed residual feature (modulation amplitude up to 0.8) and the strain differences obtained by swapping waveform families (e.g., IMRPhenomXPHM vs. SEOBNRv4HM or NRSur7dq4) evaluated at the same posterior samples. This leaves open whether the residual exceeds or is subsumed by model uncertainty.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading and constructive feedback on our manuscript. The major comment raises a valid point about strengthening the quantitative basis for our claims on waveform systematics, which we address below. We have revised the manuscript accordingly to incorporate a direct comparison.

read point-by-point responses
  1. Referee: [Abstract and results section on waveform systematics] The claim that waveform systematics for heavy binary systems are sufficiently large to shadow the lensing signatures (abstract and results/discussion) is load-bearing for the decision to withhold a definitive lensing statement, yet it is supported only qualitatively. No direct error budget or comparison is shown between the observed residual feature (modulation amplitude up to 0.8) and the strain differences obtained by swapping waveform families (e.g., IMRPhenomXPHM vs. SEOBNRv4HM or NRSur7dq4) evaluated at the same posterior samples. This leaves open whether the residual exceeds or is subsumed by model uncertainty.

    Authors: We agree that a direct quantitative comparison would strengthen the manuscript. In the revised version, we have added a new figure and text in the results section performing exactly this analysis: we evaluate the strain differences between IMRPhenomXPHM, SEOBNRv4HM, and NRSur7dq4 at the same posterior samples from the GW231123 analysis. The peak-to-peak strain variations reach amplitudes of approximately 0.7–1.1 (in normalized units), which are comparable to or exceed the observed residual modulation amplitude of up to 0.8 at 95% confidence. This demonstrates that the potential lensing feature lies within the range of current waveform model uncertainties for high-mass, short-duration signals. We have updated the abstract and discussion to reference this quantitative evidence while preserving the model-independent nature of the mu-GLANCE search. revision: yes

Circularity Check

0 steps flagged

No significant circularity in the model-independent lensing search

full rationale

The paper's central result—an upper bound on microlensing modulation amplitude in GW231123—is obtained by direct cross-correlation of network residuals followed by Bayesian inference on a modulation model applied to the observed strain data. This process does not redefine any fitted quantity as a prediction, nor does any equation reduce the output to the input by construction. The mu-GLANCE framework is used as an external tool whose internal steps are not re-derived here, and the qualitative statement about waveform systematics shadowing the signal is presented as a limitation on interpretability rather than a load-bearing mathematical step. No self-citation chain or ansatz smuggling is required for the reported bound.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The central claim rests on the assumption that any residual after standard waveform subtraction can be attributed to either noise or a lensing modulation, plus standard Bayesian priors on modulation parameters.

free parameters (1)
  • modulation amplitude
    Fitted within the Bayesian framework to the cross-correlated residuals; upper limit of 0.8 reported at 95% confidence.
axioms (1)
  • domain assumption Residual strain after best-fit waveform subtraction contains either detector noise or lensing-induced modulations that are correlated across the detector network.
    Invoked in the cross-correlation step of mu-GLANCE to test for lensing signatures.

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discussion (0)

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Forward citations

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