31 research outputs found

    Cosmography using strongly lensed gravitational waves from binary black holes

    Full text link
    Third generation gravitational wave (GW) detectors are expected to detect millions of binary black hole (BBH) mergers during their operation period. A small fraction of them (∼1%\sim 1\%) will be strongly lensed by intervening galaxies and clusters, producing multiple observable copies of the GW signals. The expected number of lensed events and the distribution of the time delay between lensed events depend on the cosmology. We develop a Bayesian analysis method for estimating cosmological parameters from the detected number of lensed events and their time delay distribution. The expected constraints are comparable to that obtained from other cosmological measurements, but probing a different redshift regime (z∼10z \sim 10) that is not explored by other probes.Comment: 9 pages, 7 figures (including supplementary material

    Waltzing binaries: Probing line-of-sight acceleration of merging compact objects with gravitational waves

    Full text link
    Line-of-sight acceleration of a compact binary coalescence (CBC) event would modulate the shape of the gravitational waves (GWs) it produces with respect to the corresponding non-accelerated CBC. Such modulations could be indicative of its astrophysical environment. We investigate the prospects of detecting this acceleration in future observing runs of the LIGO-Virgo-KAGRA network, as well as in next-generation (XG) detectors and the proposed DECIGO. We place the first observational constraints on this acceleration, for putative binary neutron star mergers GW170817 and GW190425. We find no evidence of line-of-sight acceleration in these events at 90%90\% confidence. Prospective constraints for the fifth observing run of the LIGO at A+ sensitivity suggest that accelerations for typical BNSs could be constrained with a precision of a/c∼10−7 [s−1]a/c \sim 10^{-7}~[\mathrm{s}^{-1}], assuming a signal-to-noise ratio of 1010. These improve to a/c∼10−9 [s−1]a/c \sim 10^{-9}~[\mathrm{s}^{-1}] in XG detectors, and a/c∼10−16 [s−1]a/c \sim 10^{-16}~[\mathrm{s}^{-1}] in DECIGO. We also interpret these constraints in the context of mergers around supermassive black holes.Comment: Accepted to Ap
    corecore