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First narrow-band search for continuous gravitational waves from known pulsars in advanced detector data

B. P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration)
Phys. Rev. D 96, 122006 – Published 28 December 2017; Erratum Phys. Rev. D 97, 129903 (2018)

Abstract

Spinning neutron stars asymmetric with respect to their rotation axis are potential sources of continuous gravitational waves for ground-based interferometric detectors. In the case of known pulsars a fully coherent search, based on matched filtering, which uses the position and rotational parameters obtained from electromagnetic observations, can be carried out. Matched filtering maximizes the signal-to-noise (SNR) ratio, but a large sensitivity loss is expected in case of even a very small mismatch between the assumed and the true signal parameters. For this reason, narrow-band analysis methods have been developed, allowing a fully coherent search for gravitational waves from known pulsars over a fraction of a hertz and several spin-down values. In this paper we describe a narrow-band search of 11 pulsars using data from Advanced LIGO’s first observing run. Although we have found several initial outliers, further studies show no significant evidence for the presence of a gravitational wave signal. Finally, we have placed upper limits on the signal strain amplitude lower than the spin-down limit for 5 of the 11 targets over the bands searched; in the case of J1813-1749 the spin-down limit has been beaten for the first time. For an additional 3 targets, the median upper limit across the search bands is below the spin-down limit. This is the most sensitive narrow-band search for continuous gravitational waves carried out so far.

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  • Received 6 October 2017

DOI:https://doi.org/10.1103/PhysRevD.96.122006

© 2017 American Physical Society

Physics Subject Headings (PhySH)

  1. Physical Systems
Gravitation, Cosmology & Astrophysics

Erratum

Erratum: First narrow-band search for continuous gravitational waves from known pulsars in advanced detector data [Phys. Rev. D 96, 122006 (2017)]

B. P. Abbott et al. (LIGO Scientific Collaboration and Virgo Collaboration)
Phys. Rev. D 97, 129903 (2018)

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Vol. 96, Iss. 12 — 15 December 2017

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Images

  • Figure 1
    Figure 1

    Simplified flowchart of the narrow-band search pipeline for CW. The method relies on the use of FFTs to simultaneously compute the detection statistic, for each given spin-down value, over the full explored frequency range. See [13] for more details on the method.

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  • Figure 2
    Figure 2

    Blue points: Value of the theoretical spin-down limit computed for the 11 known pulsars in our analysis, corresponding to Table 2; error bars correspond to the 1σ confidence level. Black triangles: Median over the analyzed frequency band of the upper limits on the GW amplitude, corresponding to Table 6. Red dashed line: Estimated sensitivity at 95% confidence level of a narrow-band search using data from LIGO H. Green dashed line: Estimated sensitivity at 95% confidence level of a narrow-band search using data from LIGO L.

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  • Figure 3
    Figure 3

    Top panel: SNR computed with respect to the fraction of data for the J1833-1034 outlier in the Hanford (red line), Livingston (green) and joint (blue) analysis respectively. Bottom panel: SNR computed with respect to the fraction of data for the Vela outlier in the Hanford (red line), Livingston (green) and joint (blue) analysis respectively.

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  • Figure 4
    Figure 4

    Values of the local maximum of the DS over the spin-down corrections and the frequency subbands for J1833-1034 (top panel) and Vela (bottom panel). The outliers are highlighted with the red square.

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  • Figure 5
    Figure 5

    Values of the local maximum of the DS over the spin-down corrections and the frequency subbands for a close sky position to J1833-1034 (top panel) and Vela (bottom panel).

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  • Figure 6
    Figure 6

    Plots of the 95% C.L. upper limit on the GW amplitude for the 11 pulsars. The blue dots indicate the amplitude upper limits set with our analysis; the red dashed lines indicate the theoretical spin-down limit in Table 2.

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  • Figure 7
    Figure 7

    Left: Power spectrum of Hanford (red line) and Livingston (green line) data inside the frequency region explored by the narrow-band search (blue box) around J1813-1749. Right: Power spectrum of Hanford (red line) and Livingston (green line) data inside the frequency region explored by the narrow-band search (blue box) around J1953+3252.

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  • Figure 8
    Figure 8

    Left: Histograms of the DS obtained in the J1833-1034 O2 narrow-band search for the (top) joint search, (middle) Handford search, and (bottom) Livingston search; the x-axis is normalized to the DS threshold in each search. Right: Histograms of the DS obtained in the Vela O2 narrow-band search for the (top) joint search, (middle) Handford search, and (bottom) Livingston search; the x-axis is normalized to the DS threshold in each search.

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  • Figure 9
    Figure 9

    Left: Upper limits on the GW amplitude h0 over the narrow-frequency region analyzed in O2 for J1833-1034. Right: Upper limits on the GW amplitude h0 over the narrow-frequency region analyzed in O2 for Vela.

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