ondesgravitationnelles
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* developments to higher PN, with spins and tidal effects, all needed for future detectors especially LISA. Computation of both conservative equations of motion plus effects of gravitational radiation reaction. Computation of waveforms (modes, especially the dominant quadrupole mode 22) and flux balance equations for secular evolution of the binary. | * developments to higher PN, with spins and tidal effects, all needed for future detectors especially LISA. Computation of both conservative equations of motion plus effects of gravitational radiation reaction. Computation of waveforms (modes, especially the dominant quadrupole mode 22) and flux balance equations for secular evolution of the binary. | ||
* Inclusion of eccentricity to higher PN, unbound hyperbolic orbits etc. Relation between unbound and bound (elliptical) orbits including tail effects. | * Inclusion of eccentricity to higher PN, unbound hyperbolic orbits etc. Relation between unbound and bound (elliptical) orbits including tail effects. | ||
- | * Effective Field theory techniques, amplitudes. These, together with ``classical'' | + | * Effective Field theory techniques, amplitudes. These, together with ``classical'' |
* Effective one body: under-developed in France, but crucial to match inspiral to ringdown waveforms and for practical implementation of data analysis. | * Effective one body: under-developed in France, but crucial to match inspiral to ringdown waveforms and for practical implementation of data analysis. | ||
* Numerical relativity. Tremendous progress over the last decades. A field which is under-developed in France. Connection with the community working of neutron star equations of state. | * Numerical relativity. Tremendous progress over the last decades. A field which is under-developed in France. Connection with the community working of neutron star equations of state. | ||
- | * Quasinormal modes to higher (second) order: | + | * Quasinormal modes to higher (second) order: |
- | * Recent progress on the gravitational self force problem for compact binaries, now solved numerically to second order in the mass ratio. | + | * Recent progress on the gravitational self force problem for compact binaries, now solved numerically to second order in the mass ratio, in the simplest case of the quasi-circular inspiral of nonspinning binaries. Much work remains |
- | * Study of resonances in EMRIs (extreme mass ration inspirals), and whether or not they' | + | * Study of resonances in EMRIs (extreme mass ration inspirals), and whether or not they' |
+ | * Tidal deformability of black holes in GR and alternative theories of gravity, impact on waveforms for EMRIs, tidally-induced multipole moments and test of the black hole no-hair theorem. | ||
* All these questions can be repeated in modified gravity theories, see [[gravity|Théories de gravité]], where there are many developments to refine. For the moment scalar-tensor theories (generalized Brans-Dicke) are the only ones with accurate waveforms predicted. | * All these questions can be repeated in modified gravity theories, see [[gravity|Théories de gravité]], where there are many developments to refine. For the moment scalar-tensor theories (generalized Brans-Dicke) are the only ones with accurate waveforms predicted. | ||
* Wave forms from other individual sources: important to understand other possible GW signals (continuous waves, bursts, boson stars, other exotic possibilities etc): there could well be new discoveries in the next 10 years, and one needs to be prepared. | * Wave forms from other individual sources: important to understand other possible GW signals (continuous waves, bursts, boson stars, other exotic possibilities etc): there could well be new discoveries in the next 10 years, and one needs to be prepared. | ||
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**Astrophysics, | **Astrophysics, | ||
+ | |||
+ | In the next decade the number of GW events which will be detected will rapidly increase. | ||
+ | * O4 2023-2025 -- order 1000-10^4 BBH and BNS | ||
+ | * O5 2026-2028 -- 10^5 BBH or more | ||
+ | * O6? 2030-2032 -- 10^6 BBH or more. | ||
+ | With this data, it should be possible to determine, amongst other things, the population of BH in the local universe (mass and redshift distribution), | ||
+ | Regarding Astrophysics and Cosmology: | ||
+ | |||
+ | |||
* Using individual sources to measure the Hubble constant and other cosmological parameters (e.g. equation of state of DE), see [[cosmologie|cosmologie]]. Unless there are many GW events with EM counterparts, | * Using individual sources to measure the Hubble constant and other cosmological parameters (e.g. equation of state of DE), see [[cosmologie|cosmologie]]. Unless there are many GW events with EM counterparts, | ||
* probing anisotropic expansion or the cosmological principle with GW data | * probing anisotropic expansion or the cosmological principle with GW data |
ondesgravitationnelles.1677773107.txt.gz · Last modified: 2023/03/02 17:05 by daniele.steer