2018
DOI: 10.1088/1361-6382/aab186
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On the ambiguity in relativistic tidal deformability

Abstract: Abstract. The LIGO collaboration recently reported the first gravitational-wave constraints on the tidal deformability of neutron stars. I discuss an inherent ambiguity in the notion of relativistic tidal deformability that, while too small to affect the present measurement, may become important in the future. I propose a new way to understand the ambiguity and discuss future prospects for reliably linking observed gravitational waveforms to compact object microphysics.

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Cited by 58 publications
(35 citation statements)
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“…We present below the precise late-time asymptotics away from the horizon: (1) , yield (5). The asymptotic term for ψ| r=R for outgoing perturbations in the strong field region {r = R} is consistent with the results presented in [26,29,35,39,43,52,62].…”
Section: B Asymptotics For Ernsupporting
confidence: 90%
“…We present below the precise late-time asymptotics away from the horizon: (1) , yield (5). The asymptotic term for ψ| r=R for outgoing perturbations in the strong field region {r = R} is consistent with the results presented in [26,29,35,39,43,52,62].…”
Section: B Asymptotics For Ernsupporting
confidence: 90%
“…Restricted to slowly changing tidal fields, this response can be characterized by the (dimensionless) NS tidal deformability [71] (see also Ref. [92]). Similar to the quadrupole moment scalar Q, both the second (electric-type) Love number k 2 [93] and the source-frame NS radius R S are fixed when m S and the equation of state are given.…”
Section: Pnmentioning
confidence: 99%
“…This deformation enhances GW emission and thus accelerates the decay of the quasi-circular inspiral [21][22][23]. In the post-Newtonian (PN) expansion of the inspiral dynamics [24][25][26][27][28][29][30][31][32], this effect causes the phase of the GW signal to differ from that of a binary BH from the fifth PN order onwards [21,33,34]. The leading-order contribution is proportional to each star's tidal deformability parameter, Λ = (2/3)k 2 C −5 , an EOS-sensitive quantity that describes how much a star is deformed in the presence of a tidal field.…”
Section: Introductionmentioning
confidence: 99%