V. Kalogera’s research while affiliated with Northwestern University and other places

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Publications (478)


Search for Gravitational Waves Emitted from SN 2023ixf
  • Article

May 2025

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29 Reads

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1 Citation

The Astrophysical Journal

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R. Abbott

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I. Abouelfettouh

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[...]

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J. Zweizig

We present the results of a search for gravitational-wave transients associated with core-collapse supernova SN 2023ixf, which was observed in the galaxy Messier 101 via optical emission on 2023 May 19, during the LIGO–Virgo–KAGRA 15th Engineering Run. We define a five-day on-source window during which an accompanying gravitational-wave signal may have occurred. No gravitational waves have been identified in data when at least two gravitational-wave observatories were operating, which covered ∼14% of this five-day window. We report the search detection efficiency for various possible gravitational-wave emission models. Considering the distance to M101 (6.7 Mpc), we derive constraints on the gravitational-wave emission mechanism of core-collapse supernovae across a broad frequency spectrum, ranging from 50 Hz to 2 kHz, where we assume the gravitational-wave emission occurred when coincident data are available in the on-source window. Considering an ellipsoid model for a rotating proto-neutron star, our search is sensitive to gravitational-wave energy 1 × 10 ⁻⁴ M ⊙ c ² and luminosity 2.6 × 10 ⁻⁴ M ⊙ c ² s ⁻¹ for a source emitting at 82 Hz. These constraints are around an order of magnitude more stringent than those obtained so far with gravitational-wave data. The constraint on the ellipticity of the proto-neutron star that is formed is as low as 1.08, at frequencies above 1200 Hz, surpassing past results.


Figure 6. A comparison of three different nearest-neighbor methods. For each parameter, three different histograms of errors are shown where errors are calculated using Equation (12). The blue and green histograms correspond to the proposed method with barycentric and inverse distance cubed weights, and the red corresponds to the nearest neighbor. The implementation using the inverse distance cubed as weights uses k = 4. Median values are marked within each histogram and are also indicated on the x-axis in the following order: barycentric weighting (blue), nearest neighbor (red), and d −3 (green).
Figure 7. An example of a  ( ) M log 10 transfer signal (found in the HMS-HMS grid) that is particularly difficult to interpolate due to the nonuniform morphology of nearest neighbors. In the leftmost panel, the dashed orange and blue lines correspond to the ground truth and interpolated tracks, respectively, and the colored markers on the ground truth represent the ground truth time steps used for evaluation, while the color corresponds to the severity of the error. The middle and right panels show translucent black lines that correspond to the four neighbors used for interpolation.
Figure 8. A summary of the different error types we have identified in the HMS-HMS grid. Each column corresponds to an example different error type. The top row shows the complete tracks, while the bottom row shows a zoomed-in view of the tracks. The interpolated track is shown in blue, the ground truth is shown in orange, and the nearest neighbors used are shown in black. The colored dots show the error produced at each sampled time in the ground truth.
Figure 9. A table summarizing the approximate percentage each error type contributes to the total number of high error approximations we analyzed. It should be noted that an identified high error track can exhibit more than one of each error type.
Figure 11. A histogram of the normalized age offsets of the large drops in the M 1 signal value between the predicted and ground truth HMS-HMS tracks divided by the ground truth final age.
Irregularly Sampled Time Series Interpolation for Detailed Binary Evolution Simulations
  • Article
  • Full-text available

May 2025

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10 Reads

The Astrophysical Journal

Modeling of large populations of binary stellar systems is an integral part of many areas of astrophysics, from radio pulsars and supernovae to X-ray binaries, gamma-ray bursts, and gravitational-wave mergers. Binary population synthesis codes that employ self-consistently the most advanced physics treatment available for stellar interiors and their evolution and are at the same time computationally tractable have started to emerge only recently. One element that is still missing from these codes is the ability to generate the complete time evolution of binaries with arbitrary initial conditions using precomputed three-dimensional grids of binary sequences. Here, we present a highly interpretable method, from binary evolution track interpolation. Our method implements simulation generation from irregularly sampled time series. Our results indicate that this method is appropriate for applications within binary population synthesis and computational astrophysics with time-dependent simulations in general. Furthermore, we point out and offer solutions to the difficulty surrounding evaluating the performance of signals exhibiting extreme morphologies akin to discontinuities.

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Figure 5. Percentage of BH-LMXBs formed in the different populations. The top row shows the percentage of BH-LMXBs out of all systems that avoided a CE, whereas the bottom row includes all systems in the model's population, including those that underwent a CE phase. Specific values for the bottom panel are listed in the last row of Table 2.
Figure 7. Predictions for the eccentricity of the outer orbit (e 2 ) and the spinorbit angle of the inner black hole (Ψ BH ). We color the points by the mutual inclination of the triple, which is mostly likely to be near 45° or 135° (e.g., Figure 10). If an LMXB is outlined in the plot, then it is classified as being V404 Cygni-like, meaning a 1 < 0.5 au and a 2 > 2000 au. Interestingly, the Ψ BH distribution is roughly isotropic, implying that most BH-LMXBs formed in hierarchical triples are expected to be misaligned. V404 Cygni, for example, has a likely spin-orbit misalignment, as suggested by the changing orientation of its jets (J. C. A. Miller-Jones et al. 2019). The gray and green regions, respectively, display constraints for the spin-orbit angle of the BH-LMXBs MAXI J1820+070 (J. Poutanen et al. 2022) and GRO J1655-40 (R. G. Martin et al. 2008).
Simulations Statistics
Outcomes of Triple and Binary Population Synthesis
LMXB Types at Initial Mass Transfer
Triple Evolution Pathways to Black Hole Low-mass X-Ray Binaries: Insights from V404 Cygni

April 2025

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7 Reads

The Astrophysical Journal

A recent discovery shows that V404 Cygni, a prototypical black hole low-mass X-ray binary (BH-LMXB) is a hierarchical triple: the BH and donor star are orbited by a 1.2 M ⊙ tertiary at a distance of at least 3500 au. Motivated by this system, we evolve a grid of ∼50,000 triple star systems, spanning a broad range of initial orbits. Our calculations employ MESA stellar evolution models, using POSYDON , and self-consistently track the effects of eccentric Kozai–Lidov (EKL) oscillations, mass loss, tides, and BH natal kicks. In our simulations, the progenitors of V404 Cygni-like systems have initial outer separations of 1000–10,000 au and inner separations of ∼100 au, such that they avoid Roche lobe overflow most of the time. Later on, EKL oscillations drive the inner binary to high eccentricities until tides shrink the orbit and mass transfer begins. Notably, such systems only form in simulations with very weak black hole natal kicks (≲5 km s ⁻¹ ) because stronger kicks unbind the tertiaries. Our simulations also predict a population of BH-LMXB triples that form via the classical common-envelope channel, when the BH progenitor does overflow its Roche lobe. The formation rate for this channel is also higher in triples than in isolated binaries because early EKL oscillations cause inner binaries with a wider range of initial separations to enter and survive a common envelope. Our calculations demonstrate that at least some stellar BHs form with extremely weak kicks, and that triple evolution is a significant formation channel for BH-LMXBs.


Search for Continuous Gravitational Waves from Known Pulsars in the First Part of the Fourth LIGO-Virgo-KAGRA Observing Run

April 2025

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91 Reads

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1 Citation

The Astrophysical Journal

Continuous gravitational waves (CWs) emission from neutron stars carries information about their internal structure and equation of state, and it can provide tests of general relativity. We present a search for CWs from a set of 45 known pulsars in the first part of the fourth LIGO–Virgo–KAGRA observing run, known as O4a. We conducted a targeted search for each pulsar using three independent analysis methods considering single-harmonic and dual-harmonic emission models. We find no evidence of a CW signal in O4a data for both models and set upper limits on the signal amplitude and on the ellipticity, which quantifies the asymmetry in the neutron star mass distribution. For the single-harmonic emission model, 29 targets have the upper limit on the amplitude below the theoretical spin-down limit. The lowest upper limit on the amplitude is 6.4 × 10 ⁻²⁷ for the young energetic pulsar J0537−6910, while the lowest constraint on the ellipticity is 8.8 × 10 ⁻⁹ for the bright nearby millisecond pulsar J0437−4715. Additionally, for a subset of 16 targets, we performed a narrowband search that is more robust regarding the emission model, with no evidence of a signal. We also found no evidence of nonstandard polarizations as predicted by the Brans–Dicke theory.


Figure 2. Time evolution from oRLO of the orbital period (first row), eccentricity (second row), mass ratio (third row), RLO MT rate (fourth row), the periapse separation normalized by the value at oRLO (fifth row), and the donor and CO masses (last row), for a subset of our s-eMT models with a 20 M e donor and 10 M e BH shown in Figure 1. The colors in the left column indicate various initial eccentricities and various initial orbital periods in the right column. In the mass ratio (q = M 1 / M 2 ) we have indicated with horizontal lines at q = 1 (black) and q = 0.76 (gray dashed) approximate transition points in the sign of  a eMT from Equation (9) and  e eMT from Equation (10). Red points in the q panels denote when each model reaches TAMS (thick to thin line transitions in Figure 1), which occurs at different times owing to the different r p,i and t oRLO for each model.
Mass Transfer in Eccentric Orbits with Self-consistent Stellar Evolution

April 2025

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2 Reads

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1 Citation

The Astrophysical Journal

We investigate Roche lobe overflow mass transfer (MT) in eccentric binary systems between stars and compact objects (COs), modeling the coupled evolution of both the star and the orbit due to eccentric MT (eMT) in a self-consistent framework. We implement the analytic expressions for secular rates of change of the orbital semimajor axis and eccentricity, assuming a delta function MT at periapse, in the binary stellar evolution code MESA . Two scenarios are examined: (1) a simplified model isolating the effects of eMT on stellar and orbital evolution, and (2) realistic binary configurations that include angular momentum exchange (e.g., tides, mass loss, spin–orbit coupling, and gravitational-wave (GW) radiation). Unlike the ad hoc approach of instant circularization that is often employed, explicit modeling of eMT reveals that a large fraction of binaries can remain eccentric post-MT. Even binaries that naturally circularize during eMT have different properties (donor mass and orbital size) compared to predictions from instant circularization, with some showing fundamentally different evolutionary outcomes (e.g., stable vs. unstable MT). We demonstrate that a binary’s initial mass ratio and eccentricity are predictive of whether it will remain eccentric or circularize after eMT. These findings underscore the importance of eMT in understanding CO-hosting binary populations, including X-ray binaries, GW sources, and other high-energy transients.



Figure 1. The primary ZAMS masses of all NSBH progenitors in our S16 and F12d fiducial populations. The differing mass ranges between prescriptions are a result of how each computes remnant masses and assigns CO types (Section 3.1).
Figure 3. The number of NSBH binaries in the F12d and S16 fiducial populations that form through Channel I (pink) vs. Channel II (green) (Sections 3.2.2 and 3.2.3). We show the subset of binaries in each channel that merge in a Hubble time (solid) and those that do not merge, or remain detached (hatched).
Figure 5. BH vs. NS masses for all NSBH binaries at their formation in both the F12d (black) and S16 (green/pink) fiducial populations. Each population is separated into binaries that merge and do not merge in a Hubble time with the large and small symbols, respectively. For the S16 population, the NSBHs are also separated by Channel I vs. Channel II formation (Sections 3.2.2 and 3.2.3). All F12d NSBHs form through Channel I.
Challenges in Forming Millisecond Pulsar–Black Holes from Isolated Binaries

March 2025

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10 Reads

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2 Citations

The Astrophysical Journal

Binaries harboring a millisecond pulsar (MSP) and a black hole (BH) are a key observing target for current and upcoming pulsar surveys. We model the formation and evolution of such binaries in isolation at solar metallicity using the next-generation binary population synthesis code POSYDON . We examine neutron star (NS)–BH binaries where the NS forms first (labeled NSBH), as the NS must be able to spin up to MSP rotation periods before the BH forms in these systems. We find that NSBHs are very rare and have a birth rate <1 Myr ⁻¹ for a Milky Way–like galaxy in our typical models. The NSBH formation rate is 2–3 orders of magnitude smaller than that for NS–BH binaries where the BH forms first (labeled BHNS). These rates are also sensitive to model assumptions about the supernova (SN) remnant masses, natal kicks, metallicity, and common-envelope (CE) evolution parameters. We find that 100% of NSBHs undergo a mass ratio reversal before the first SN and up to 52% of NSBHs undergo a double CE phase after the mass ratio reversal occurs. Most importantly, no NSBH binaries in our populations undergo a mass transfer phase, either stable or unstable, after the first SN. This implies that there is no possibility of pulsar spin-up via accretion, and thus MSP–BH binaries cannot form. Thus, dynamical environments and processes may provide the only formation channels for such MSP–BH binaries.


Swift-BAT GUANO Follow-up of Gravitational-wave Triggers in the Third LIGO–Virgo–KAGRA Observing Run

February 2025

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81 Reads

The Astrophysical Journal

We present results from a search for X-ray/gamma-ray counterparts of gravitational-wave (GW) candidates from the third observing run (O3) of the LIGO–Virgo–KAGRA network using the Swift Burst Alert Telescope (Swift-BAT). The search includes 636 GW candidates received with low latency, 86 of which have been confirmed by the offline analysis and included in the third cumulative Gravitational-Wave Transient Catalogs (GWTC-3). Targeted searches were carried out on the entire GW sample using the maximum-likelihood Non-imaging Transient Reconstruction and Temporal Search pipeline on the BAT data made available via the GUANO infrastructure. We do not detect any significant electromagnetic emission that is temporally and spatially coincident with any of the GW candidates. We report flux upper limits in the 15–350 keV band as a function of sky position for all the catalog candidates. For GW candidates where the Swift-BAT false alarm rate is less than 10 ⁻³ Hz, we compute the GW–BAT joint false alarm rate. Finally, the derived Swift-BAT upper limits are used to infer constraints on the putative electromagnetic emission associated with binary black hole mergers.


Structure and Skewness of the Effective Inspiral Spin Distribution of Binary Black Hole Mergers

January 2025

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2 Reads

The detection of gravitational waves has brought to light a population of binary black holes that merge within a Hubble time. Multiple formation channels can contribute to this population, making it difficult to definitively associate particular population features with underlying stellar physics. Black hole spins are considered an important discriminator between various channels, but they are less well-measured than masses, making conclusive astrophysical statements using spins difficult thus far. In this paper, we consider the distribution of the effective inspiral spin χeff\chi_{\rm eff} -- a quantity much better measured than individual component spins. We show that non-Gaussian features like skewness, asymmetry about zero, and multimodality can naturally arise in the χeff\chi_{\rm eff} distribution when multiple channels contribute to the population. Searching for such features, we find signs of skewness and asymmetry already in the current catalogs, but no statistically significant signs of bimodality. These features provide robust evidence for the presence of a subpopulation with spins preferentially aligned to the binary's orbital angular momentum; and we conservatively estimate the fraction of this subpopulation to be at least 12%17%12 \% - 17\% (at 90%90\% credibility). Our models do not find an excess of non-spinning systems and instead find that at least 20%\sim 20 \% of the binaries have some degree of negative χeff\chi_{\rm eff}. The data also suggest that, if preferentially aligned mergers form a significant fraction of the population, they must have small spins.


Table 2 (continued)
Figure 4. 95% credible upper limits on ellipticity ε 95% and mass quadrupole Q 95% 22
Figure 6. Blue stars show the ratio between the O4a h0 upper limits for the analyzed targets (excluding the glitching pulsars) assuming the single-harmonic model divided by the corresponding h0 upper limits in Abbott et al. (2022) for the Bayesian method as a function of the corresponding frequency at twice the rotation frequency (red circles refer instead to the C21 parameter at the rotation frequency assuming the dual-harmonic model). Blue filled stars show the h0 upper limit ratios considering the targets (J0205+6449, J0737−3039A, J1813−1246, J1831−0952, J1837−0604) analyzed using O2 (Abbott et al. 2019c) and O1 data (blue asterisk for J1826−1334, Abbott et al. (2017b)).
Table of the results for the targeted search on the set of 45 known pulsars for the three considered pipelines described in Section 3.
Search for continuous gravitational waves from known pulsars in the first part of the fourth LIGO-Virgo-KAGRA observing run

January 2025

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197 Reads

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1 Citation

Continuous gravitational waves (CWs) emission from neutron stars carries information about their internal structure and equation of state, and it can provide tests of General Relativity. We present a search for CWs from a set of 45 known pulsars in the first part of the fourth LIGO--Virgo--KAGRA observing run, known as O4a. We conducted a targeted search for each pulsar using three independent analysis methods considering the single-harmonic and the dual-harmonic emission models. We find no evidence of a CW signal in O4a data for both models and set upper limits on the signal amplitude and on the ellipticity, which quantifies the asymmetry in the neutron star mass distribution. For the single-harmonic emission model, 29 targets have the upper limit on the amplitude below the theoretical spin-down limit. The lowest upper limit on the amplitude is 6.4 ⁣× ⁣10276.4\!\times\!10^{-27} for the young energetic pulsar J0537-6910, while the lowest constraint on the ellipticity is 8.8 ⁣× ⁣1098.8\!\times\!10^{-9} for the bright nearby millisecond pulsar J0437-4715. Additionally, for a subset of 16 targets we performed a narrowband search that is more robust regarding the emission model, with no evidence of a signal. We also found no evidence of non-standard polarizations as predicted by the Brans-Dicke theory.


Citations (59)


... Recent advances in observational technology have provided new insights into NS properties, driving intense scientific interest and activity [18][19][20][21][22][23][24]. Recycled millisecond pulsars undergoing starquakes show a sudden increase in gravitational wave amplitude, providing a unique signature of NS matter at high densities [25][26][27][28]. These breakthroughs have inspired innovative research spanning multiple disciplines, leveraging collaborative and interdisciplinary approaches development. ...

Reference:

Inferring the Equation of State from Neutron Star Observables via Machine Learning
Search for Continuous Gravitational Waves from Known Pulsars in the First Part of the Fourth LIGO-Virgo-KAGRA Observing Run
  • Citing Article
  • April 2025

The Astrophysical Journal

... Moreover, recent theoretical work has argued for eccentricity retention during mass transfer in long period, roughly equal mass binaries (Rocha et al. 2024), as well as eccentricity pumping due to phase dependent Roche-lobe overflow (Sepinsky et al. 2007(Sepinsky et al. , 2009(Sepinsky et al. , 2010 or in post-mass transfer binaries due to the presence of a circumbinary disk (Vos et al. 2015;Valli et al. 2024). Given this, we might expect the true population of pre-collapse binaries to be circularized due to mass transfer up to a limiting period, above which systems can retain more eccentricity (Rocha et al. 2024). ...

Mass Transfer in Eccentric Orbits with Self-consistent Stellar Evolution

The Astrophysical Journal

... For the vast majority of binaries that evolve to become NSBHs (≳ 95 %; F. S. Broekgaarden et al. 2021;Z. Xing et al. 2024;C. Liotine et al. 2025), the BH is expected to form first from the more massive primary star (m 1 ), while the progenitor of the NS is still on the MS (m 2 ). This implies an intermediate evolutionary stage of an inner binary with a BH and an OB-type stellar companion ("BHOB triple"). We thus construct a twostage binary evolution model for the inner binaries, ...

Challenges in Forming Millisecond Pulsar–Black Holes from Isolated Binaries

The Astrophysical Journal

... Some of them are repeating, and some of them are not. The first FRB was discovered in 2007 25 , Upper limits on emitted GW energy (EGW) and energy of radio bursts (E radio ), reproduced from10 . The upper limits on GW energy have improved 5 orders of magnitude thanks to a close distance of SGR 1935+2154, but the constraints on the GW to radio energy ratio improved only slightly. ...

A Search Using GEO600 for Gravitational Waves Coincident with Fast Radio Bursts from SGR 1935+2154

The Astrophysical Journal

... To contextualize the potential of such a detector, a 30 kg SLedDoG with λ Φ ¼ 1 and a run time of 10 7 s would be sensitive to monochromatic, coherent GWs with h ∼ 10 −24 at ∼10 kHz-MHz frequencies. Such a sensitivity could, for instance, probe gravitational radiation from superradiant axion clouds around stellar-mass black holes in the Milky Way [66] and inspirals of primordial black holes with masses 10 −12 M ⊙ ≲ m PBH ≲ 10 −7 M ⊙ [67]. We note, however, that such statements relating strain sensitivity to BSM physics are highly model dependent. ...

Simulating the Galactic population of axion clouds around stellar-origin black holes: Gravitational wave signals in the 10–100 kHz band
  • Citing Article
  • December 2024

Physical Review D

... Additionally, this expanded state only lasts 1-100 years (185). Given the limited mass involved and the short duration of the inflated phase, according to recent models of eccentric mass transfer the effect on the orbit should be minimal (187). ...

Mass Transfer in Eccentric Orbits with Self-consistent Stellar Evolution

... In this paper, we use the POSYDON population synthesis code Andrews et al. 2024) to examine the possible formation channels of isolated Galactic NS-BH binaries that host recycled NSs, regardless of whether they become potential GW sources or not. As previously mentioned, the NSs in these binaries are expected to form first so that they may accrete from their companions and be spun-up before the BH forms. ...

POSYDON Version 2: Population Synthesis with Detailed Binary-Evolution Simulations across a Cosmological Range of Metallicities

... Many binary population synthesis (BPS) studies have previously examined isolated NS-BH formation with a focus on their properties as gravitational wave (GW) sources (Kruckow et al. 2018;Mapelli & Giacobbo 2018;Shao & Li 2018;Broekgaarden et al. 2021;Chattopadhyay et al. 2021;Román-Garza et al. 2021;Drozda et al. 2022;Xing et al. 2023Xing et al. , 2024. Growing interest in this area of research is related to the GW detections consistent with being the products of NS-BH coalescences that have been recently reported by the LIGO-Virgo-KAGRA (LVK) collaboration. ...

Mass-gap Black Holes in Coalescing Neutron Star Black Hole Binaries

... In the case of a massive binary with two stellar components, mass loss near L2 has been predicted as a likely outcome (Podsiadlowski et al. 1992) and the specific angular momentum of the outflow has been noted as an important uncertainty (Wellstein et al. 2001). Gallegos-Garcia et al. (2024) (see also Lu et al. 2023) show that, when the accretor is much more massive than the donor, the specific angular momentum lost through winds launched from the outer accretion disk can also be much larger than that of the accretor's orbit. ...

Angular Momentum Loss during Stable Mass Transfer onto a Compact Object: The Effect of Mass Loss via Accretion Disk Winds

The Astrophysical Journal

... Searches for eccentric subsolar binaries have also been performed [49,50]. Unmodeled [51,52] and modeled [53] searches have been performed for eccentric stellar-mass BBH systems. While these searches did not yield any new candidates, they constrained the local merger rate to be less than: 1700 mergers Gpc −3 yr −1 for BNS systems with e 10 ≤ 0.43 and 0.33 mergers Gpc −3 yr −1 for BBH systems with total mass M ∈ ½70M ⊙ ; 200M ⊙ and e 15 < 0.3 at 90% confidence. ...

Search for Eccentric Black Hole Coalescences during the Third Observing Run of LIGO and Virgo
  • Citing Article
  • September 2024

The Astrophysical Journal