Abstract

A fundamental quantity in signal analysis is the metric $g_{ab}$ on parameter space, which quantifies the fractional "mismatch" $m$ between two (time- or frequency-domain) waveforms. When searching for weak gravitational-wave or electromagnetic signals from sources with unknown parameters $\lambda$ (masses, sky locations, frequencies, etc.) the metric can be used to create and/or characterize "template banks". These are grids of points in parameter space; the metric is used to ensure that the points are correctly separated from one another. For small coordinate separations $d\lambda^a$ between two points in parameter space, the traditional ansatz for the mismatch is a quadratic form $m=g_{ab} d\lambda^a d\lambda^b$. This is a good approximation for small separations but at large separations it diverges, whereas the actual mismatch is bounded. Here we introduce and discuss a simple "spherical" ansatz for the mismatch $m=\sin^2(\sqrt{g_{ab} d\lambda^a d\lambda^b})$. This agrees with the metric ansatz for small separations, but we show that in simple cases it provides a better (and bounded) approximation for large separations, and argue that this is also true in the generic case. This ansatz should provide a more accurate approximation of the mismatch for semi-coherent searches, and may also be of use when creating grids for hierarchical searches that (in some stages) operate at relatively large mismatch.

Highlights

  • More than two decades ago, when the first generation of interferometric gravitational-wave (GW) detectors was still in the planning stages, a handful of pioneers investigated the techniques that would be needed to detect GW signals [1,2,3,4,5,6,7,8,9,10]

  • If the template is normalized, ðT; TÞ 1⁄4 1, ρ is called the signal-to-noise ratio (SNR). This is reviewed in a signal-processing context in Refs. [18] and [19] and in the GW context in Refs. [20] and [21]

  • The solution to the second problem is to construct the SNR ρ in Eq (1.1) for many different templates Tλi, where λ are the parameters that describe the waveform and the integer i labels a finite set of distinct points which are being sampled from parameter space [3,10,11,16,24,25,26,27,28,29,30,31,32,33]

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Summary

INTRODUCTION

More than two decades ago, when the first generation of interferometric gravitational-wave (GW) detectors was still in the planning stages, a handful of pioneers investigated the techniques that would be needed to detect GW signals [1,2,3,4,5,6,7,8,9,10]. The parameters describing the signals (such as the object masses in a binary system or the rotation frequency and spindown rate of a neutron star) were not known. This required repeated searches for signals with many different parameter combinations, creating a significant computational challenge. If the template is normalized, ðT; TÞ 1⁄4 1, ρ is called the signal-to-noise ratio (SNR). This is reviewed in a signal-processing context in Refs. If the detector noise is colored [11], the inner product is most expressed in the frequency domain as ðA; BÞ

A ÃðfÞBðfÞ SðjfjÞ df: ð1:3Þ
MISMATCH AND THE METRIC APPROXIMATION TO THE MISMATCH
METRIC APPROXIMATION AND THE SPHERICAL APPROXIMATION
SIMPLE ILLUSTRATIVE EXAMPLE
SECOND EXAMPLE
THIRD EXAMPLE
SIGNIFICANCE AND IMPACT
Findings
VIII. CONCLUSION
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