B. D. O'Brien’s research while affiliated with University of Florida and other places

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Publications (168)


Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network
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July 2024

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104 Reads

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54 Citations

The Astrophysical Journal

R. Abbott

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Gravitational lensing by massive objects along the line of sight to the source causes distortions to gravitational wave (GW) signals; such distortions may reveal information about fundamental physics, cosmology, and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO-Virgo network. We search for repeated signals from strong lensing by (1) performing targeted searches for subthreshold signals, (2) calculating the degree of overlap among the intrinsic parameters and sky location of pairs of signals, (3) comparing the similarities of the spectrograms among pairs of signals, and (4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by (1) frequency-independent phase shifts in strongly lensed images, and (2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the nondetection of GW lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.

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Search for Gravitational-wave Transients Associated with Magnetar Bursts in Advanced LIGO and Advanced Virgo Data from the Third Observing Run

April 2024

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178 Reads

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20 Citations

The Astrophysical Journal

Gravitational waves are expected to be produced from neutron star oscillations associated with magnetar giant flares and short bursts. We present the results of a search for short-duration (milliseconds to seconds) and long-duration (∼100 s) transient gravitational waves from 13 magnetar short bursts observed during Advanced LIGO, Advanced Virgo, and KAGRA’s third observation run. These 13 bursts come from two magnetars, SGR 1935+2154 and Swift J1818.0−1607. We also include three other electromagnetic burst events detected by Fermi-GBM which were identified as likely coming from one or more magnetars, but they have no association with a known magnetar. No magnetar giant flares were detected during the analysis period. We find no evidence of gravitational waves associated with any of these 16 bursts. We place upper limits on the rms of the integrated incident gravitational-wave strain that reach 3.6 × 10 ⁻²³ / Hz at 100 Hz for the short-duration search and 1.1 × 10 ⁻²² / Hz at 450 Hz for the long-duration search. For a ringdown signal at 1590 Hz targeted by the short-duration search the limit is set to 2.3 × 10 ⁻²² / Hz . Using the estimated distance to each magnetar, we derive upper limits on the emitted gravitational-wave energy of 1.5 × 10 ⁴⁴ erg (1.0 × 10 ⁴⁴ erg) for SGR 1935+2154 and 9.4 × 10 ⁴³ erg (1.3 × 10 ⁴⁴ erg) for Swift J1818.0−1607, for the short-duration (long-duration) search. Assuming isotropic emission of electromagnetic radiation of the burst fluences, we constrain the ratio of gravitational-wave energy to electromagnetic energy for bursts from SGR 1935+2154 with the available fluence information. The lowest of these ratios is 4.5 × 10 ³ .


A Joint Fermi-GBM and Swift-BAT Analysis of Gravitational-wave Candidates from the Third Gravitational-wave Observing Run

March 2024

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119 Reads

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11 Citations

The Astrophysical Journal

We present Fermi Gamma-ray Burst Monitor (Fermi-GBM) and Swift Burst Alert Telescope (Swift-BAT) searches for gamma-ray/X-ray counterparts to gravitational-wave (GW) candidate events identified during the third observing run of the Advanced LIGO and Advanced Virgo detectors. Using Fermi-GBM onboard triggers and subthreshold gamma-ray burst (GRB) candidates found in the Fermi-GBM ground analyses, the Targeted Search and the Untargeted Search, we investigate whether there are any coincident GRBs associated with the GWs. We also search the Swift-BAT rate data around the GW times to determine whether a GRB counterpart is present. No counterparts are found. Using both the Fermi-GBM Targeted Search and the Swift-BAT search, we calculate flux upper limits and present joint upper limits on the gamma-ray luminosity of each GW. Given these limits, we constrain theoretical models for the emission of gamma rays from binary black hole mergers.


Search for Gravitational Waves Associated with Fast Radio Bursts Detected by CHIME/FRB during the LIGO–Virgo Observing Run O3a

September 2023

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329 Reads

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22 Citations

The Astrophysical Journal

We search for gravitational-wave (GW) transients associated with fast radio bursts (FRBs) detected by the Canadian Hydrogen Intensity Mapping Experiment Fast Radio Burst Project, during the first part of the third observing run of Advanced LIGO and Advanced Virgo (2019 April 1 15:00 UTC–2019 October 1 15:00 UTC). Triggers from 22 FRBs were analyzed with a search that targets both binary neutron star (BNS) and neutron star–black hole (NSBH) mergers. A targeted search for generic GW transients was conducted on 40 FRBs. We find no significant evidence for a GW association in either search. Given the large uncertainties in the distances of our FRB sample, we are unable to exclude the possibility of a GW association. Assessing the volumetric event rates of both FRB and binary mergers, an association is limited to 15% of the FRB population for BNS mergers or 1% for NSBH mergers. We report 90% confidence lower bounds on the distance to each FRB for a range of GW progenitor models and set upper limits on the energy emitted through GWs for a range of emission scenarios. We find values of order 10 ⁵¹ –10 ⁵⁷ erg for models with central GW frequencies in the range 70–3560 Hz. At the sensitivity of this search, we find these limits to be above the predicted GW emissions for the models considered. We also find no significant coincident detection of GWs with the repeater, FRB 20200120E, which is the closest known extragalactic FRB.


Figure 1. The FPPs of each lensed candidate pair constructed from the set of GW events that exceed an astrophysical probability (Farr et al. 2015; Kapadia et al. 2020) threshold of 0.5, as evaluated using the B L U and ML classification statistics. Orange dashed lines that correspond to an FPP threshold of 10 −2 , are also placed. Pairs whose B L U -based or ML-based FPPs fall below this threshold are selected for additional joint parameter estimation analyses. B L U < 10 −6 has been mapped to an FPP of 1, which is reflected in the gap along the vertical axis between 0.4 and 1.
Figure 4. Distribution of microlensing log 10 Bayes factors B Micro U for all events in O3 (blue, solid line) and simulated unlensed signals (orange, dashed line) from Abbott et al. (2021a). bution of log 10 B Micro U for all the events in O3 and simulated unlensed signals from Abbott et al. (2021a). The distribution of log 10 B Micro U is primarily clustered around 0 and the distribution for O3 events does not extend to significantly higher values than the distribution for simulated signals. The marginalized posteriors of the microlensing parameters are shown in Appendix B. We conclude that there is no compelling evidence for the presence of microlensing signatures.
Figure 5. Merger rate density as a function of redshift based on the GWTC-3 results without lensing constraints (grey) and with lensing constraints (cross-hatching) included. For clarity, we show only the results for galaxy-scale lenses. Because lensed detections may occur at higher redshifts than unlensed events, their non-observation can be used to constrain the rate of mergers at higher redshifts. The 'No lensing' results shown here do not include constraints derived from the absence of an SGWB. The latter constraints are shown separately by the solid black curves.
Figure 6. The spread in the 90% upper limits on f DM obtained from the O3 events using 5 different redshift distribution models for BBH mergers: Belczynski et al. (2016),Dominik et al. (2013), Madau & Dickinson (2014), Abbott et al. (2021j) and uniform in comoving 4-volume, assuming a monochromatic mass spectrum for the compact objects forming dark matter. The lens mass is shown on the horizontal axis. The grey (black) shaded regions correspond to the spread in f DM upper bounds computed assuming flat (Jeffreys) prior on Λ and Λ . The upper and lower curves bounding the spreads correspond to the most pessimistic (weakest) and optimistic (strongest) upper limits, as determined from the set of assumed redshift distributions, in each mass bin.
Figure 10. Marginalized posterior distributions of redshifted lens mass M z L and log 10 B Micro U between microlensed and unlensed hypotheses.
Search for gravitational-lensing signatures in the full third observing run of the LIGO-Virgo network

April 2023

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493 Reads

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9 Citations

Gravitational lensing by massive objects along the line of sight to the source causes distortions of gravitational wave-signals; such distortions may reveal information about fundamental physics, cosmology and astrophysics. In this work, we have extended the search for lensing signatures to all binary black hole events from the third observing run of the LIGO--Virgo network. We search for repeated signals from strong lensing by 1) performing targeted searches for subthreshold signals, 2) calculating the degree of overlap amongst the intrinsic parameters and sky location of pairs of signals, 3) comparing the similarities of the spectrograms amongst pairs of signals, and 4) performing dual-signal Bayesian analysis that takes into account selection effects and astrophysical knowledge. We also search for distortions to the gravitational waveform caused by 1) frequency-independent phase shifts in strongly lensed images, and 2) frequency-dependent modulation of the amplitude and phase due to point masses. None of these searches yields significant evidence for lensing. Finally, we use the non-detection of gravitational-wave lensing to constrain the lensing rate based on the latest merger-rate estimates and the fraction of dark matter composed of compact objects.


Population of Merging Compact Binaries Inferred Using Gravitational Waves through GWTC-3

March 2023

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245 Reads

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939 Citations

Physical Review X

We report on the population properties of compact binary mergers inferred from gravitational-wave observations of these systems during the first three LIGO-Virgo observing runs. The Gravitational-Wave Transient Catalog 3 (GWTC-3) contains signals consistent with three classes of binary mergers: binary black hole, binary neutron star, and neutron star–black hole mergers. We infer the binary neutron star merger rate to be between 10 and 1700 Gpc − 3 yr − 1 and the neutron star–black hole merger rate to be between 7.8 and 140 Gpc − 3 yr − 1 , assuming a constant rate density in the comoving frame and taking the union of 90% credible intervals for methods used in this work. We infer the binary black hole merger rate, allowing for evolution with redshift, to be between 17.9 and 44 Gpc − 3 yr − 1 at a fiducial redshift ( z = 0.2 ). The rate of binary black hole mergers is observed to increase with redshift at a rate proportional to ( 1 + z ) κ with κ = 2. 9 − 1.8 + 1.7 for z ≲ 1 . Using both binary neutron star and neutron star–black hole binaries, we obtain a broad, relatively flat neutron star mass distribution extending from 1.2 − 0.2 + 0.1 to 2.0 − 0.3 + 0.3 M ⊙ . We confidently determine that the merger rate as a function of mass sharply declines after the expected maximum neutron star mass, but cannot yet confirm or rule out the existence of a lower mass gap between neutron stars and black holes. We also find the binary black hole mass distribution has localized over- and underdensities relative to a power-law distribution, with peaks emerging at chirp masses of 8.3 − 0.5 + 0.3 and 27.9 − 1.8 + 1.9 M ⊙ . While we continue to find that the mass distribution of a binary’s more massive component strongly decreases as a function of primary mass, we observe no evidence of a strongly suppressed merger rate above approximately 60 M ⊙ , which would indicate the presence of a upper mass gap. Observed black hole spins are small, with half of spin magnitudes below χ i ≈ 0.25 . While the majority of spins are preferentially aligned with the orbital angular momentum, we infer evidence of antialigned spins among the binary population. We observe an increase in spin magnitude for systems with more unequal-mass ratio. We also observe evidence of misalignment of spins relative to the orbital angular momentum. Published by the American Physical Society 2023


Figure 4. Selection of follow-up threshold as a function of GW frequency. If the data contained no signal and only Gaussian noise, each template in the parameter space would have some chance of producing a statistic value exceeding a given threshold. Within each 5 Hz frequency band, the total number of templates was computed and used to find the threshold at which the expected number of Gaussian outliers above that value would be 0.1. This is shown with short blue lines for the templates in the present search (see Table 3); for reference, the thresholds calculated from the numbers of templates in the O1 search of Abbott et al. (2017c) are shown in orange. Because of the more efficient template placement of algorithm from Wagner et al. (2022), the O3 search has fewer templates, and therefore a lower implied threshold, than the O1 search, which used the same coherence times. The exception is for 400 Hz < f 0 < 600 Hz, where the same threshold of 6.2 was used for the O1 and O3 searches, and the latter used twice the coherence time (and therefore a denser parameter space lattice) as the former. The present search uses a threshold of 6.3 for 25 Hz < f 0 < 400 Hz and 5.8 for 600 Hz < f 0 < 1600 Hz (black dashed line), which are lower than in the O1 search (magenta dashed line). Note that the large number of non-Gaussian outliers (see Table 3) makes the Gaussian follow-up level an imprecise tool in any event.
Figure 7. Comparison of upper limits to predictions of torque balance models. The gray band indicates the h 0 upper limit implied by the h 0 eff upper limit in the bottom panel of Figure 6, assuming the range of possible inclinations from  0c o s 1 i . (Linear polarization (cos 0 i = ) is at the top, and circular polarization (cos 1 i = ) is at the bottom.) The dashed blue line is the usual conservative torque balance estimate assuming accretion at the surface of the NS, r = R * = 10 km. The dotted-dashed red line is the same model assuming a lever arm of r = r A ≈ 49 km, which is the value of the Alfvén radius given by Equation (10) for ξ = 1 and B = 10 8 G. Note that this is slightly larger than the value of 35 km used in, e.g., Zhang et al. (2021) and Abbott et al. (2022a), since we use the inferred mass accretion rate of Sco X-1. The colored bands show the range of predictions for the models of Glampedakis & Suvorov (2021), in particular model 2, for the range of 0.3 < ξ < 0.5, assuming a magnetic field of 10 8 G (GS8) or 10 9 G (GS9).
Observed Parameters of the LMXB Sco X-1
Parameters Used for the Cross-correlation Search
Model-based cross-correlation search for gravitational waves from the low-mass X-ray binary Scorpius X-1 in LIGO O3 data

December 2022

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281 Reads

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13 Citations

The Astrophysical Journal Letters

We present the results of a model-based search for continuous gravitational waves from the low-mass X-ray binary Scorpius X-1 using LIGO detector data from the third observing run of Advanced LIGO and Advanced Virgo. This is a semicoherent search that uses details of the signal model to coherently combine data separated by less than a specified coherence time, which can be adjusted to balance sensitivity with computing cost. The search covered a range of gravitational-wave frequencies from 25 to 1600 Hz, as well as ranges in orbital speed, frequency, and phase determined from observational constraints. No significant detection candidates were found, and upper limits were set as a function of frequency. The most stringent limits, between 100 and 200 Hz, correspond to an amplitude h0 of about 10−25 when marginalized isotropically over the unknown inclination angle of the neutron star's rotation axis, or less than 4 × 10−26 assuming the optimal orientation. The sensitivity of this search is now probing amplitudes predicted by models of torque balance equilibrium. For the usual conservative model assuming accretion at the surface of the neutron star, our isotropically marginalized upper limits are close to the predicted amplitude from about 70 to 100 Hz; the limits assuming that the neutron star spin is aligned with the most likely orbital angular momentum are below the conservative torque balance predictions from 40 to 200 Hz. Assuming a broader range of accretion models, our direct limits on gravitational-wave amplitude delve into the relevant parameter space over a wide range of frequencies, to 500 Hz or more.


Figure 1. Sensitive volume-time as a function of the source frame chirp mass in data from O3, obtained through the analysis of the set of common injections (blue triangles with dotted lines, orange circles with dashed lines, and green squares with continuous lines). The statistical errors are evaluated at 90% confidence interval, following Eq. (2) and represented by the shaded areas.
Figure 4. Constraints on DM fraction of PBHs, f PBH , for a monochromatic mass function and assuming the merger rates for early PBH binaries from Hütsi et al. (2021) (orange) and late PBH binaries from Phukon et al. (2021) (blue). Shown in black are results for SSM searches in O2 (Abbott et al. 2019b) with and without the rate suppression factor fsup. For the first time, f PBH = 1 for early binaries is excluded in the whole SSM range probed by this search.
Figure 5. Constraints on the abundance of DBHs, f DBH , as a function of the lower limit of the DBH mass distribution, M DBH min from O3 data for the 3 search pipelines: GstLAL (dotted), MBTA (dashed) and PyCBC (solid). Constraints from the search for SSM compact objects in O3a data (Abbott et al. 2022) are shown for comparison.
Search for subsolar-mass black hole binaries in the second part of Advanced LIGO's and Advanced Virgo's third observing run

December 2022

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204 Reads

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1 Citation

We describe a search for gravitational waves from compact binaries with at least one component with mass 0.2 MM_\odot -- 1.0M1.0 M_\odot and mass ratio q0.1q \geq 0.1 in Advanced LIGO and Advanced Virgo data collected between 1 November 2019, 15:00 UTC and 27 March 2020, 17:00 UTC. No signals were detected. The most significant candidate has a false alarm rate of 0.2 yr1\mathrm{yr}^{-1}. We estimate the sensitivity of our search over the entirety of Advanced LIGO's and Advanced Virgo's third observing run, and present the most stringent limits to date on the merger rate of binary black holes with at least one subsolar-mass component. We use the upper limits to constrain two fiducial scenarios that could produce subsolar-mass black holes: primordial black holes (PBH) and a model of dissipative dark matter. The PBH model uses recent prescriptions for the merger rate of PBH binaries that include a rate suppression factor to effectively account for PBH early binary disruptions. If the PBHs are monochromatically distributed, we can exclude a dark matter fraction in PBHs fPBH0.6f_\mathrm{PBH} \gtrsim 0.6 (at 90% confidence) in the probed subsolar-mass range. However, if we allow for broad PBH mass distributions we are unable to rule out fPBH=1f_\mathrm{PBH} = 1. For the dissipative model, where the dark matter has chemistry that allows a small fraction to cool and collapse into black holes, we find an upper bound fDBH<105f_{\mathrm{DBH}} < 10^{-5} on the fraction of atomic dark matter collapsed into black holes.


Figure 1. Cumulative distribution of the p-values of the most significant clusters found by the short-duration searches. The expectation value and 90% band are calculated as in (Abbott et al. 2022); the expectation value is calculated assuming a uniform distribution of p-values (given by the null hypothesis), with the corresponding 90% confidence band shown by the shaded region. The lowest p-value in the delayed on-source search is 3.5 × 10 −3 from burst 2653, and is determined to be most likely an instrumental artifact through arguments invoking both astrophysics and the characteristics of the detector. Several centered on-source search clusters fall outside of the 90% band, but many of them have properties inconsistent with what one would expect from an astrophysical source, so this is likely a result of small number statistics. Although the most significant of these, which appears in burst 2656, has p-value 8.6 × 10 −3 and a peak frequency (1577 Hz) which is consistent with expectations for an f-mode, we provide arguments for why this is not the case in Sec. 3.1.
Figure 3. Spectrograms of the LHO (left) and LLO (right) data around the time of the most significant cluster found by the centered-window short-duration search of burst 2656. Even though the cluster is only barely visible in LLO data, these spectrograms show that the ambient noise in each detector is in a normal state around the time of the flare.
Search for gravitational-wave transients associated with magnetar bursts in Advanced LIGO and Advanced Virgo data from the third observing run

October 2022

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380 Reads

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4 Citations

Gravitational waves are expected to be produced from neutron star oscillations associated with magnetar giant flares and short bursts. We present the results of a search for short-duration (milliseconds to seconds) and long-duration (\sim 100 s) transient gravitational waves from 13 magnetar short bursts observed during Advanced LIGO, Advanced Virgo and KAGRA's third observation run. These 13 bursts come from two magnetars, SGR 1935+2154 and Swift J1818.0-1607. We also include three other electromagnetic burst events detected by Fermi GBM which were identified as likely coming from one or more magnetars, but they have no association with a known magnetar. No magnetar giant flares were detected during the analysis period. We find no evidence of gravitational waves associated with any of these 16 bursts. We place upper bounds on the root-sum-square of the integrated gravitational-wave strain that reach 2.2×10232.2 \times 10^{-23} /Hz/\sqrt{\text{Hz}} at 100 Hz for the short-duration search and 8.7×10238.7 \times 10^{-23} /Hz/\sqrt{\text{Hz}} at 450 Hz for the long-duration search, given a detection efficiency of 50%. For a ringdown signal at 1590 Hz targeted by the short-duration search the limit is set to 1.8×10221.8 \times 10^{-22} /Hz/\sqrt{\text{Hz}}. Using the estimated distance to each magnetar, we derive upper bounds on the emitted gravitational-wave energy of 3.2×10433.2 \times 10^{43} erg (7.3×10437.3 \times 10^{43} erg) for SGR 1935+2154 and 8.2×10428.2 \times 10^{42} erg (2.8×10432.8 \times 10^{43} erg) for Swift J1818.0-1607, for the short-duration (long-duration) search. Assuming isotropic emission of electromagnetic radiation of the burst fluences, we constrain the ratio of gravitational-wave energy to electromagnetic energy for bursts from SGR 1935+2154 with available fluence information. The lowest of these ratios is 3×1033 \times 10^3.


FIG. 1. Uncertainty ellipses corresponding to 1σ (blue line), 2σ (yellow line), and 3σ (green line), for T asc and P. Top: the curves at the reference time T 0 , when T asc;ref is uncorrelated with P 0 or its uncertainties. Bottom: the effect of propagating T asc;ref and P 0 , with their respective uncertainties, to the start of O3 (T O3;0 ¼ 1238166483 GPS time) (solid lines) or the end of O3 (T O3end ¼ 1269361423 GPS time) (black dots). T asc;0 represents the central value of T asc;ref propagated to the start or end of O3; that is, T asc;0 is different for the solid and dotted lines. In both panels we have P 0 ¼ 68023.86048 s.
FIG. 3. Candidates plotted as a function of their terminating frequency bin q à ðt N T Þ (horizontal axis, units in hertz) and the orbital parameters a 0 (vertical axis in left panel, units in seconds), offset from the central time of ascension T asc − T asc 0 (vertical axis in central panel; units in seconds) and offset from the central period P − P 0 (vertical axis in right panel; units in seconds). The color scale indicates the maxðLÞ obtained for the candidate. Candidates marked with purple squares are eliminated by the single IFO veto, while red circles mark the ones eliminated by the known lines veto. The candidate with no marking survives both the single IFO and known lines vetoes, but is eliminated by its absence when using noise-subtracted data (see Sec. IVA).
FIG. 4. Frequentist effective wave strain upper limits at 95% confidence as a function of subband frequency, for three scenarios: circular polarization with ι ¼ 0 (blue stars), ι ≈ 44° based on the electromagnetic measurements (see Ref. [51]; orange dots), and a flat prior on cos ι (green dots). Indirect torque-balance upper limits (see Sec. V C) for two torque lever arms are also shown: the stellar radius (red solid line) and the Alfvén radius (dashed red line).
Search for gravitational waves from Scorpius X-1 with a hidden Markov model in O3 LIGO data

September 2022

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215 Reads

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41 Citations

Physical Review D

Results are presented for a semicoherent search for continuous gravitational waves from the low-mass x-ray binary Scorpius X-1, using a hidden Markov model (HMM) to allow for spin wandering. This search improves on previous HMM-based searches of Laser Interferometer Gravitational-Wave Observatory data by including the orbital period in the search template grid, and by analyzing data from the latest (third) observing run. In the frequency range searched, from 60 to 500 Hz, we find no evidence of gravitational radiation. This is the most sensitive search for Scorpius X-1 using a HMM to date. For the most sensitive subband, starting at 256.06 Hz, we report an upper limit on gravitational wave strain (at 95% confidence) of h095%=6.16×10−26, assuming the orbital inclination angle takes its electromagnetically restricted value ι=44°. The upper limits on gravitational wave strain reported here are on average a factor of ∼3 lower than in the second observing run HMM search. This is the first Scorpius X-1 HMM search with upper limits that reach below the indirect torque-balance limit for certain subbands, assuming ι=44°.


Citations (67)


... This difference has sparked ongoing discussions about how to classify GW lensing into strong and microlensing regimes [9][10][11]. While no definitive detection of lensed GWs has been reported to date [12][13][14], the advent of next-generation ground-and space-based detectors promises to greatly enhance the prospects for such observations [15,16], potentially enabling the use of GW lensing as a novel probe of the environments surrounding their sources [17,18]. ...

Reference:

Lense-Thirring Precession Modulates Repeated Lensing of Continues Gravitational Wave Source from AGN Disks
Search for Gravitational-lensing Signatures in the Full Third Observing Run of the LIGO–Virgo Network

The Astrophysical Journal

... Previous work has performed targeted searches for sources observed electromagnetically or through neutrinos (e.g., Abbott et al. 2024Abbott et al. , 2022aAbbasi et al. 2023;Abbott et al. 2022b). There are also all-sky and all-time searches to ensure that no gravitationalwave burst event is missed if there are no electromagnetic counterparts (Abbott et al. 2021d,c). ...

Search for Gravitational-wave Transients Associated with Magnetar Bursts in Advanced LIGO and Advanced Virgo Data from the Third Observing Run

The Astrophysical Journal

... No gravitational signal was found in association neither to Fast Radio Bursts detected by CHIME/FRB during O3a [32], nor to magnetar bursts during O3 [38]. In addition, the joint Fermi-GBM and Swift-BAT Analysis [106] and the Swift-BAT GUANO follow-up [178] of gravitational candidates during O3 run were negative. The search for coincident optical, high energy candidates in Swift observations and gravitational candidates was negative [132]. ...

A Joint Fermi-GBM and Swift-BAT Analysis of Gravitational-wave Candidates from the Third Gravitational-wave Observing Run

The Astrophysical Journal

... Active searches to find time-coincident events in these two domains are therefore needed, e.g. [90,91]. Searching for the association of FRBs with GWs is currently inefficient, primarily due to the following reasons. ...

Search for Gravitational Waves Associated with Fast Radio Bursts Detected by CHIME/FRB during the LIGO–Virgo Observing Run O3a

The Astrophysical Journal

... Indeed, the detection methodologies are entirely different from those of electromagnetic-wave detection, owing to the nature of the detectors (laser interferometers [23][24][25][26] vs. optical telescopes) and the signals (gravitational wave vs. electromagnetic). Given the recent collaboration searches for gravitational-wave lensing triggered by promising forecasts, the development of new technologies and a worldwide hunt [10,[27][28][29][30][31][32][33][34][35][36][37], it is important to understand the general strategies for gravitationalwave lensing searches and detection and how they differ from strategies employed in the electromagnetic frontiers. ...

Search for gravitational-lensing signatures in the full third observing run of the LIGO-Virgo network

... To date, four versions of the catalog have been released: GWTC-1 [7], GWTC-2 [8], GWTC-2.1 [9], and GWTC-3 [10]. These help inform results related to testing the theory of general relativity [11][12][13][14], cosmology [15,16], black hole properties and formation mechnisms [17][18][19], and binary population and merger rates [20][21][22]. ...

Population of Merging Compact Binaries Inferred Using Gravitational Waves through GWTC-3

Physical Review X

... As discussed in 11 , deriving firm conclusions about the NS equation of state or magnetic field strength from our upper limits is challenging without assuming a specific accretion model. The resulting sensitivity estimation versus frequency results are shown in Figure 1, where it is also shown the theoretical strain (at the torque-balance level) assuming M NS = 1.4M ⊙ and ...

Model-based cross-correlation search for gravitational waves from the low-mass X-ray binary Scorpius X-1 in LIGO O3 data

The Astrophysical Journal Letters

... After analyzing the lensing parameter space in Section II, we selected a specific subset of lensing parameters, which includes three frequencies and three lens masses for simulation, see Appendix B for details. The reference strain for the simulated CW signals is set to h o = 10 −25 , based on the upper limits of h o set in the 100-200 Hz range during the first three LVK observing runs [89]. In the following, we adopt for the standard deviation of the noise the value σ n = 0.0002, the representative noise strain amplitude n o = 10 −20 , based on the current overall quality of the data. ...

Searches for Gravitational Waves from Known Pulsars at Two Harmonics in the Second and Third LIGO-Virgo Observing Runs

The Astrophysical Journal

... For instance, a variety of theories beyond standard model physics predict the existence of ultralight dark matter, with masses m b 1 eV. Recently, the proposal that boson clouds could form around spinning black holes through the superradiance mechanism and emit CWs [31] has received growing interest, and searches during the last advanced LIGO/Virgo O3 run have already been performed [32]. ...

All-sky search for gravitational wave emission from scalar boson clouds around spinning black holes in LIGO O3 data
  • Citing Article
  • May 2022

... Black holes (BHs) have gained significant attention in recent times. The two major milestones of modern physics that have propelled the growing interest in the field of BH physics are the discovery of gravitational waves (GWs) by the LIGO and Virgo team in 2015 [1][2][3][4][5][6], and the first ever image of the BH M87 * at the center of M87 galaxy, by the Event Horizon Telescope (EHT) group in 2019 [7][8][9][10][11][12]. Since then a lot of efforts have been directed towards a better understanding of the physics of BHs. ...

Search for continuous gravitational wave emission from the Milky Way center in O3 LIGO-Virgo data
  • Citing Article
  • August 2022