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Targeted search for the kinematic dipole of the gravitational-wave background

Adrian Ka-Wai Chung, Alexander C. Jenkins, Joseph D. Romano, and Mairi Sakellariadou
Phys. Rev. D 106, 082005 – Published 21 October 2022

Abstract

There is growing interest in using current and future gravitational-wave interferometers to search for anisotropies in the gravitational-wave background. One guaranteed anisotropic signal is the kinematic dipole induced by our peculiar motion with respect to the cosmic rest frame, as measured in other full-sky observables such as the cosmic microwave background. Our prior knowledge of the amplitude and direction of this dipole is not explicitly accounted for in existing searches by LIGO/Virgo/KAGRA but could provide crucial information to help disentangle the sources which contribute to the gravitational-wave background. Here, we develop a targeted search pipeline which uses this prior knowledge to enable unbiased and minimum-variance inference of the dipole magnitude. Our search generalizes existing methods to allow for a time-dependent signal model, which captures the annual modulation of the dipole due to the Earth’s orbit. We validate our pipeline on mock data, demonstrating that neglecting this time dependence can bias the inferred dipole by as much as O(10%). We then run our analysis on the full LIGO/Virgo O1+O2+O3 dataset, obtaining upper limits on the dipole amplitude that are consistent with existing anisotropic search results.

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  • Received 3 August 2022
  • Accepted 28 September 2022

DOI:https://doi.org/10.1103/PhysRevD.106.082005

© 2022 American Physical Society

Physics Subject Headings (PhySH)

Gravitation, Cosmology & Astrophysics

Authors & Affiliations

Adrian Ka-Wai Chung1,*, Alexander C. Jenkins2,†, Joseph D. Romano3,‡, and Mairi Sakellariadou1,§

  • 1Theoretical Particle Physics and Cosmology Group, Physics Department, King’s College London, University of London, Strand, London WC2R 2LS, United Kingdom
  • 2Department of Physics and Astronomy, University College London, London WC1E 6BT, United Kingdom
  • 3Department of Physics and Astronomy, Texas Tech University, Box 41051, Lubbock, Texas 79409-1051, USA

  • *ka-wai.chung@ligo.org
  • alex.jenkins@ucl.ac.uk
  • joseph.d.romano@ttu.edu
  • §mairi.sakellariadou@kcl.ac.uk

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Vol. 106, Iss. 8 — 15 October 2022

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Images

  • Figure 1
    Figure 1

    The kinematic dipole is a superposition between a (time-independent) solar dipole and a (time-dependent) orbital dipole. Here, we show the orbital dipole at 0, 2, 4, and 6 months from the time at which the Earth is at perihelion (reading from top to bottom), with the amplitude of the total dipole becoming progressively smaller over this time. The resulting O(10%) variation is difficult to distinguish by eye here but has a significant impact on the search, as demonstrated in Fig. 2.

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  • Figure 2
    Figure 2

    Relative error of our targeted kinematic dipole search as a function of observing time for simulated data containing a kinematic dipole signal Dα=3.1×108 for α=0 (top panel), Dα=2.3×108 for α=2/3 (middle panel), and Dα=4×109 for α=3 (bottom panel). The blue and red traces correspond to analyses using the full (time-dependent) dipole template and the (time-independent) solar dipole template, respectively. While the relative errors for the full dipole template analyses converge to zero rapidly, those obtained using the solar-dipole template show a relative error consistent with the expected error (48) (dashed red line).

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  • Figure 3
    Figure 3

    Forecast upper limits (95% confidence) on the dipole amplitude with a third-generation interferometer network (Einstein Telescope+two Cosmic Explorers). The predicted dipole from compact binary coalescences is, in principle, accessible with less than two days of data.

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