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    Tidal Love numbers of neutron stars in Horndeski theories

    Robin Fynn Diedrichs1,*, Shinji Tsujikawa2,†, and Kent Yagi3,‡

    • 1Institute for Theoretical Physics, Goethe University, 60438 Frankfurt am Main, Germany
    • 2Department of Physics, Waseda University, 3-4-1 Okubo, Shinjuku, Tokyo 169-8555, Japan
    • 3Department of Physics, University of Virginia, Charlottesville, Virginia 22904, USA

    • *Contact author: diedrichs@itp.uni-frankfurt.de
    • †Contact author: tsujikawa@waseda.jp
    • ‡Contact author: ky5t@Virginia.edu

    Phys. Rev. D 112, 044023 – Published 13 August, 2025

    DOI: https://doi.org/10.1103/cmb4-chn3

    Abstract

    Precision measurements of the gravitational wave signal from compact binary inspirals allow us to constrain the internal structure of those objects via physical parameters such as the tidal Love numbers. In scalar-tensor theories, one typically finds new types of Love numbers that are usually not considered or simply absent in general relativity, which further allows us to constrain deviations from general relativity. Building upon previous results, we present the linear perturbation equations necessary to calculate static and even-parity tidal Love numbers in Horndeski theories, the most general scalar-tensor theories with second-order field equations of motion. We further focus on the quadrupolar Love numbers and demonstrate how these can be extracted from the asymptotic expansion of the perturbation fields. We find that there is a potential ambiguity in extracting the Love numbers in this way, which we resolve by performing supplementary calculations in the effective field theory framework. We show that, in the case of scalar-tensor theories, the tidal Love numbers are not directly given by the 1/r3 term in the asymptotic expansion of the perturbation fields, as there is an additional contribution to this term independent of the Love numbers. We calculate such a contribution for a minimally coupled scalar field and also for the Damour-Esposito-Farèse model. For the latter, we find that the Love numbers can differ by O(1∼10)%, if this additional contribution is not taken into account.

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