Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (2024)

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Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors

Hanlin Song, Dicong Liang, Ziming Wang, and Lijing Shao
Phys. Rev. D 109, 123014 – Published 7 June 2024
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Abstract

Stochastic gravitational-wave (GW) background (SGWB) contains information about the early Universe and astrophysical processes. The recent evidence of SGWB by pulsar timing arrays in the nanohertz band is a breakthrough in the GW astronomy. For ground-based GW detectors, while in data analysis, the SGWB can be masked by loud GW events from compact binary coalescences (CBCs). Assuming a next-generation ground-based GW detector network, we investigate the potential for detecting the astrophysical and cosmological SGWB with non-CBC origins by subtracting recovered foreground signals of loud CBC events. The Fisher Information Matrix (FIM) method is adopted for quick calculation. As an extension of the previous studies, two more essential features are considered. Firstly, we incorporate nonzero aligned or antialigned spin parameters in our waveform model. Because of the inclusion of spins, we obtain significantly more pessimistic results than the previous work, where the residual energy density of foreground is even larger than the original CBC foreground. For the most extreme case, we observe that the subtraction results are approximately 10 times worse for binary black hole events and 20 times worse for binary neutron star events than the scenarios without accounting for spins. The degeneracy between the spin parameters and the symmetric mass ratio is strong in the parameter estimation process, and it contributes most to the imperfect foreground subtraction. Secondly, in this work, extreme CBC events with condition numbers of FIMs cΓ>1015 are preserved. The impacts of these extreme events on foreground subtraction are discussed. Our results have important implications for assessing the detectability of SGWB from non-CBC origins for ground-based GW detectors.

  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (1)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (2)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (3)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (4)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (5)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (6)
  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (7)
  • Received 1 January 2024
  • Accepted 13 May 2024

DOI:https://doi.org/10.1103/PhysRevD.109.123014

© 2024 American Physical Society

Physics Subject Headings (PhySH)

Gravitation, Cosmology & Astrophysics

Authors & Affiliations

Hanlin Song1, Dicong Liang2,3, Ziming Wang2, and Lijing Shao2,4,*

  • *lshao@pku.edu.cn

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Vol. 109, Iss. 12 — 15 June 2024

Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (8)
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Images

  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (12)

    Figure 1

    Results from treatment (i) for 9-d PE for BBHs (upper left) and BNSs (lower left), and 11-d PE for BBHs (upper right) and BNSs (lower right). Each subfigure shows the total GW energy spectrum Ωtot in black solid line and two components (Ωns and Ωerr) of the residual GW energy spectrum for different ρthr. Ωns (dashed line) comes from the events that are not subtracted while Ωerr (dash-dotted line) comes from the imperfect subtraction of the CBC foreground. For a direct check, the two panels on the left reproduce the results of Fig.2 in Zhou etal. [44] for the IMRPhenomD waveform.

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (13)

    Figure 2

    Same as Fig.1, but for treatment (ii).

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (14)

    Figure 3

    Subfigure (a)shows number density distribution of the relative ratio Rrel and subfigure (b)shows absolute ratio Rabs. Both subfigures show results for the BNS 9-d PE case with ρthr=12. Plots for events with high/low cΓ values (denoted with red/blue color) are shown separately. Three frequency bins are chosen for illustration. The distributions at 10, 100, 200, 400, 800, and 2000Hz have similar features, which are not shown here.

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (15)

    Figure 4

    Parameter distributions of events with high and low cΓ values in four PE cases. In this figure, we set ρthr=8 for BBH cases and ρthr=12 for BNS cases. We show three parameters here: chirp mass in the observer frame Mz, symmetric mass ratio η, and orbital inclination angle ι. Red color denotes events with cΓ>1015, while gray color denotes events with cΓ<1015.

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (16)

    Figure 5

    Contribution from each parameter to Ωerr for BBHs (left panel) and BNSs (right panel). Each subfigure shows Ωerr from 11-d PE results (black solid line) and contribution from each parameter (dashed line). We choose ρthr equal to 8 and 12 for BBHs and BNSs respectively.

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (17)

    Figure 6

    Subfigure (a)shows the relative ratio Rrel and subfigure (b)shows absolute ratio Rrel. Both subfigures show results for 9-d PE (blue line) and 11-d PE (red line) of BBHs. We set ρthr=8 and choose three frequency bins to illustrate. The BNS case has a similar feature in our simulation, which is not shown here.

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  • Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (18)

    Figure 7

    The foreground subtraction results are presented for the main method (from main text) with red color and the supplementary method (from this Appendix) with blue color. The left panels show the results for 9-d PE, while the right panels show the results for 11-d PE. In the top panels, each subfigure shows the Ωtot with solid line and Ωerr with ρthr=8 with a dash-dotted line. In the bottom panels, each subfigure shows the results of Ωerr against Ωtot.

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Impact of spin in compact binary foreground subtraction for estimating the residual stochastic gravitational-wave background in ground-based detectors (2024)
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