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Monitoring of Continuous-Wave Hardware Injections in LIGO Interferometers during the O4 Observing Run

Preet Baxi, Jessica Leviton, Eilam Morag, Matthew Pitkin, Keith Riles

TL;DR

This work documents a triad of monitoring approaches for LIGO CW hardware injections during O4: a highly templated template-generation method, a conventional F-statistic analysis, and a Bayesian inference framework. Together, they validate detector response, absolute timing, and data cleaning by reconstructing injected signals across a broad frequency range and multiple detectors, achieving phase-coherent recovery over billions of cycles. The results demonstrate small systematic biases consistent with calibration uncertainties, precise amplitude and phase recovery for strong injections, and robust posterior distributions for source parameters, reinforcing end-to-end CW search reliability. The study provides essential end-to-end validation that enhances confidence in sustained coherent CW searches and informs calibration and gating practices for future observing runs.

Abstract

Although there have now been hundreds of transient gravitational-wave detections of merging compact stars by the LIGO-Virgo-KAGRA (LVK) detector network, no continuous-wave (CW) signals have yet been discovered. To ensure that such signals, expected to be exceedingly weak, can be detected in the ongoing O4 observing run by coherent integration over years, simulated waveforms ('hardware injections') are injected directly into the LIGO data by continuously modulating the positions of the interferometer mirrors so as to mimic nearly sinusoidal signals from fast-spinning galactic neutron stars. A set of 18 such simulated CW sources are injected with signal frequencies spanning much of the LIGO detection band and with varying sky locations. By verifying the successful recovery of the simulated signals, including preservation of absolute phase over as many as 10^{11} signal cycles, we validate our understanding of detector response and end-to-end search pipelines, including data cleaning. Daily and weekly monitoring of the signal reconstruction is meant to catch any unexpected sudden changes in interferometer response, to verify that signal-to-noise ratio increases as expected and to verify that simulated source parameters are recovered correctly. We describe three methods of monitoring: 1) a highly templated matched filter to extract signal amplitude and phase precisely; 2) a frequentist Fstatistic evaluation that marginalizes over amplitude, phase and orientation of the star; and 3) a Bayesian reconstruction of the source parameters together with noise characterization. Results from each method are shown, with emphasis on the new templated method, which yields precise measurement of the critical phase offset parameter and therefore validates understanding of absolute timing delays in the detector response and data stream.

Monitoring of Continuous-Wave Hardware Injections in LIGO Interferometers during the O4 Observing Run

TL;DR

This work documents a triad of monitoring approaches for LIGO CW hardware injections during O4: a highly templated template-generation method, a conventional F-statistic analysis, and a Bayesian inference framework. Together, they validate detector response, absolute timing, and data cleaning by reconstructing injected signals across a broad frequency range and multiple detectors, achieving phase-coherent recovery over billions of cycles. The results demonstrate small systematic biases consistent with calibration uncertainties, precise amplitude and phase recovery for strong injections, and robust posterior distributions for source parameters, reinforcing end-to-end CW search reliability. The study provides essential end-to-end validation that enhances confidence in sustained coherent CW searches and informs calibration and gating practices for future observing runs.

Abstract

Although there have now been hundreds of transient gravitational-wave detections of merging compact stars by the LIGO-Virgo-KAGRA (LVK) detector network, no continuous-wave (CW) signals have yet been discovered. To ensure that such signals, expected to be exceedingly weak, can be detected in the ongoing O4 observing run by coherent integration over years, simulated waveforms ('hardware injections') are injected directly into the LIGO data by continuously modulating the positions of the interferometer mirrors so as to mimic nearly sinusoidal signals from fast-spinning galactic neutron stars. A set of 18 such simulated CW sources are injected with signal frequencies spanning much of the LIGO detection band and with varying sky locations. By verifying the successful recovery of the simulated signals, including preservation of absolute phase over as many as 10^{11} signal cycles, we validate our understanding of detector response and end-to-end search pipelines, including data cleaning. Daily and weekly monitoring of the signal reconstruction is meant to catch any unexpected sudden changes in interferometer response, to verify that signal-to-noise ratio increases as expected and to verify that simulated source parameters are recovered correctly. We describe three methods of monitoring: 1) a highly templated matched filter to extract signal amplitude and phase precisely; 2) a frequentist Fstatistic evaluation that marginalizes over amplitude, phase and orientation of the star; and 3) a Bayesian reconstruction of the source parameters together with noise characterization. Results from each method are shown, with emphasis on the new templated method, which yields precise measurement of the critical phase offset parameter and therefore validates understanding of absolute timing delays in the detector response and data stream.
Paper Structure (18 sections, 27 equations, 15 figures, 2 tables)

This paper contains 18 sections, 27 equations, 15 figures, 2 tables.

Figures (15)

  • Figure 1: Cumulative SNR measurements for Injection 6 and Injection 8 from H1 and L1 detectors. The first row corresponds to H1 data, while the second row represents L1 data. Adjacent error bars in these cumulative graphs are highly correlated.
  • Figure 2: Weighted average $h_0$ by SFT for Injection 6 and Injection 8. The first row shows H1 data, while the second row represents L1 data.
  • Figure 3: Cumulative phase offset reconstructions for Injection 6 (left panels) and Injection 8 (right panels) from the H1 and L1 detectors. The top panels correspond to H1 data, while the bottom panels depict L1 data. Within each panel, the top graph shows the cosine projection of the reconstructed amplitude, the middle graph shows the sine projection, and the bottom graph shows the inferred phase offset. Ideally, the cosine projection should agree with the intended injected $h_0$ shown, and the sine projection should be consistent with zero. The intended $h_0$ is shown on the sine graphs for scale.
  • Figure 4: Relative phase offset of recovered signal for Injection 6 and Injection 8 from H1 and L1 detectors. The first row corresponds to H1 data, while the second row represents L1 data. Each column highlights the comparative performance across different metrics for the two pulsars.
  • Figure 5: Weighted average $h_0$ plots for H1 and L1 detectors for all injections.
  • ...and 10 more figures