TY - JOUR
T1 - New approach to template banks of gravitational waves with higher harmonics
T2 - Reducing matched-filtering cost by over an order of magnitude
AU - Wadekar, Digvijay
AU - Venumadhav, Tejaswi
AU - Mehta, Ajit Kumar
AU - Roulet, Javier
AU - Olsen, Seth
AU - Mushkin, Jonathan
AU - Zackay, Barak
AU - Zaldarriaga, Matias
N1 - Publisher Copyright: © 2024 American Physical Society.
PY - 2024/10/15
Y1 - 2024/10/15
N2 - Searches for gravitational wave events use models, or templates, for the signals of interest. The templates used in current searches in the LIGO-Virgo-KAGRA data model the dominant quadrupole mode (ℓ,|m|)=(2,2) of the signals and omit subdominant higher-order modes (HMs) such as (ℓ,|m|)=(3,3), (4, 4), which are predicted by general relativity. This omission reduces search sensitivity to black hole mergers in interesting parts of parameter space, such as systems with high masses and asymmetric-mass ratios. We develop a new strategy to include HMs in template banks: instead of making templates containing a combination of different modes, we separately store normalized templates corresponding to (2, 2), (3, 3), and (4, 4) modes. To model aligned-spin (3, 3), (4, 4) waveforms corresponding to a given (2, 2) waveform, we use a combination of post-Newtonian formulas and machine learning tools. In the matched-filtering stage, one can filter each mode separately with the data and collect the time series of signal-to-noise ratios (SNRs). This leads to a HM template bank whose matched-filtering cost is just ≈3× that of a quadrupole-only search (as opposed to ≈100× in previously proposed HM search methods). Our method is effectual and generally applicable for template banks constructed with either stochastic or geometric placement techniques. New gravitational wave candidate events that we detect using our HM banks and details for combining the different SNR mode time series are presented in accompanying papers [D. Wadekar et al., arXiv:2312.06631; D. Wadekar et al., Phys. Rev. D 110, 044063 (2024)PRVDAQ2470-001010.1103/PhysRevD.110.044063]. Additionally, we discuss nonlinear compression of (2, 2)-only geometric placement template banks using machine learning algorithms.
AB - Searches for gravitational wave events use models, or templates, for the signals of interest. The templates used in current searches in the LIGO-Virgo-KAGRA data model the dominant quadrupole mode (ℓ,|m|)=(2,2) of the signals and omit subdominant higher-order modes (HMs) such as (ℓ,|m|)=(3,3), (4, 4), which are predicted by general relativity. This omission reduces search sensitivity to black hole mergers in interesting parts of parameter space, such as systems with high masses and asymmetric-mass ratios. We develop a new strategy to include HMs in template banks: instead of making templates containing a combination of different modes, we separately store normalized templates corresponding to (2, 2), (3, 3), and (4, 4) modes. To model aligned-spin (3, 3), (4, 4) waveforms corresponding to a given (2, 2) waveform, we use a combination of post-Newtonian formulas and machine learning tools. In the matched-filtering stage, one can filter each mode separately with the data and collect the time series of signal-to-noise ratios (SNRs). This leads to a HM template bank whose matched-filtering cost is just ≈3× that of a quadrupole-only search (as opposed to ≈100× in previously proposed HM search methods). Our method is effectual and generally applicable for template banks constructed with either stochastic or geometric placement techniques. New gravitational wave candidate events that we detect using our HM banks and details for combining the different SNR mode time series are presented in accompanying papers [D. Wadekar et al., arXiv:2312.06631; D. Wadekar et al., Phys. Rev. D 110, 044063 (2024)PRVDAQ2470-001010.1103/PhysRevD.110.044063]. Additionally, we discuss nonlinear compression of (2, 2)-only geometric placement template banks using machine learning algorithms.
UR - http://www.scopus.com/inward/record.url?scp=85208375494&partnerID=8YFLogxK
U2 - 10.1103/PhysRevD.110.084035
DO - 10.1103/PhysRevD.110.084035
M3 - مقالة
SN - 2470-0010
VL - 110
JO - Physical review D
JF - Physical review D
IS - 8
M1 - 084035
ER -