30 mars 2021 à 1 avril 2021
Institut Henri Poincaré
Fuseau horaire Europe/Paris

Session

Contributed talks: Waveforms

30 mars 2021, 09:30

Documents de présentation

Aucun document.

  1. Dr Alexandre Le Tiec (Observatoire de Paris)
    30/03/2021 09:30
    FORMES D’ONDE

    The open question of whether a black hole can become tidally deformed by an external gravitational field has profound implications for fundamental physics, astrophysics and gravitational-wave astronomy. Love tensors characterize the tidal deformability of compact objects such as astrophysical (Kerr) black holes under an external static tidal field. We prove that all Love tensors vanish...

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  2. Adrien Kuntz (Scuola Normale Superiore, Pisa)
    30/03/2021 09:45
    FORMES D’ONDE

    The three body-problem, even in the simple Newtonian case, exhibits very rich dynamical behaviors. The study of a hierachical configuration, in which a close inner binary is orbited by a distant perturber, has been initiated by Lidov and Kozai in the 60's. The eccentricity oscillations that they discovered is particularly relevant to gravitational wave astronomy. On the other hand, several...

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  3. Stavros Mougiakakos (IPhT,CEA-Saclay)
    30/03/2021 10:00
    FORMES D’ONDE

    We derive the static Schwarzschild-Tangherlini metric by extracting the classical contributions from the multiloop vertex functions of a graviton emitted from a massive scalar field. At each loop order the classical contribution is proportional to a unique master integral given by the massless sunset integral. By computing the scattering amplitudes up to three-loop order in general dimension,...

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  4. Massimiliano Maria Riva
    30/03/2021 10:15
    FORMES D’ONDE

    We study the gravitational radiation emitted during the scattering of two spinless bodies in the post-Minkowskian Effective Field Theory approach. We derive the conserved stress-energy tensor linearly coupled to gravity and the classical probability amplitude of graviton emission at leading and next-to-leading order in the Newton’s constant $G$. The amplitude can be expressed in compact
    form...

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