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Galileon Gravity vs dRGT Massive Gravity
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Galileon Gravity Rejected | dRGT Massive Gravity Speculative | |
|---|---|---|
| Proposed | 2009 | 2011 |
| Key figures | Alberto Nicolis, Riccardo Rattazzi, Enrico Trincherini | Claudia de Rham, Gregory Gabadadze, Andrew Tolley |
| In one sentence | Gravity gains an extra field, taken from the DGP braneworld, that can accelerate the expansion while switching itself off near stars and planets. | De Rham, Gabadadze and Tolley gave the graviton a tiny mass without the Boulware-Deser ghost that sank earlier attempts, but the theory's simplest cosmological solutions are still unstable. |
| Predictions |
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| Where it breaks |
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| Key unresolved problem | The speed-of-gravity problem: the quartic and quintic terms that let the Galileon fit cosmological data also change the speed of gravitational waves, and the cubic version alone fails the ISW test. | The missing-cosmology problem: the constraint that removes the ghost also forbids a flat expanding universe, and the curved ones that remain are unstable. |
| Reader vote | No votes yet | No votes yet |
Galileon Gravity
2009 · Rejected
dRGT Massive Gravity
2011 · Speculative
Proposed
2009
2011
Key figures
Alberto Nicolis, Riccardo Rattazzi, Enrico Trincherini
Claudia de Rham, Gregory Gabadadze, Andrew Tolley
In one sentence
Gravity gains an extra field, taken from the DGP braneworld, that can accelerate the expansion while switching itself off near stars and planets.
De Rham, Gabadadze and Tolley gave the graviton a tiny mass without the Boulware-Deser ghost that sank earlier attempts, but the theory's simplest cosmological solutions are still unstable.
Predictions
- Late-time acceleration driven by the Galileon field, with no [[cosmological constant]]
- In the cubic version, gravitational potentials deepen at late times, which flips the sign of the correlation between [[cosmic microwave background]] temperature and nearby galaxies
- In the quartic and quintic versions, gravitational waves travel at a speed different from light at low redshift
- The extra force is screened inside the solar system and other gravitationally bound systems
- Gravity has a finite range set by the graviton mass, with a Yukawa-type fall-off at the largest distances
- Gravitational waves of different frequencies travel at slightly different speeds, because massive gravitons disperse
- On some self-accelerating branches, an effective cosmological constant proportional to the graviton mass squared drives late-time acceleration
- Near massive bodies, the Vainshtein mechanism hides the extra modes and recovers the predictions of general relativity
Where it breaks
- Once coupled to curved spacetime, the covariant Galileon keeps the Galileon interactions but breaks the exact galilean symmetry that defined the original model.
- Fits need a non-zero neutrino mass to match the data reasonably, around 0.5 eV in Renk and colleagues' analysis.
- Peirone and colleagues (2018) compared Bayesian evidence with ΛCDM and found covariant Galileon models strongly disfavoured by cosmological data.
- D'Amico and colleagues (2011) showed that the constraint removing the ghost also forbids exactly homogeneous and isotropic universes.
- De Felice, Gumrukcuoglu and Mukohyama (2012) found every homogeneous and isotropic solution unstable, with at least one ghost.
- The self-accelerating open universes have no exactly flat limit, so the theory jumps discontinuously as spatial curvature goes to zero.
Key unresolved problem
The speed-of-gravity problem: the quartic and quintic terms that let the Galileon fit cosmological data also change the speed of gravitational waves, and the cubic version alone fails the ISW test.
The missing-cosmology problem: the constraint that removes the ghost also forbids a flat expanding universe, and the curved ones that remain are unstable.
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