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Strong coupling and bounds on the spin-2 mass in massive gravity
Clare Burrage1, Nemanja Kaloper, Antonio Padilla
1School of Physics and Astronomy, University of Nottingham, Nottingham NG7 2RD, United Kingdom.
The de Rham-Gabadadze-Tolley theory for a massive spin-2 field has a low cutoff due to higher-derivative interactions. This research derives mass bounds for this massive graviton theory to remain perturbative.
Area of Science:
- Theoretical Physics
- Gravitational Theories
- Particle Physics
Background:
- The de Rham-Gabadadze-Tolley (dRGT) theory describes a single massive spin-2 field.
- This theory generically possesses a cutoff scale significantly below the Planck scale.
- This low cutoff arises from higher-derivative self-interactions of extra modes in the massive spin-2 multiplet.
Purpose of the Study:
- To investigate the perturbative viability of the dRGT massive spin-2 theory.
- To derive bounds on the mass of the massive spin-2 field.
- To determine the conditions under which the theory can be considered a valid description of massive gravity.
Main Methods:
- Analysis of higher-derivative self-interactions in the dRGT theory.
- Calculation of the effective cutoff scale, considering environmental effects and the graviton mass.
- Derivation of mass bounds by imposing perturbativity down to millimeter scales.
Main Results:
- The effective cutoff of the dRGT theory is dependent on environmental parameters and the massive spin-2 field's mass.
- For the theory to be perturbative down to millimeter scales, the massive spin-2 field mass is constrained to be approximately ≳O(1) meV in the generic case.
- Weaker bounds are found in scenarios involving fine-tuning.
Conclusions:
- The dRGT theory of a single massive spin-2 field is best understood as a theory of nonlinear propagation on a fixed background.
- It does not serve as a general approximation to Einstein's theory of general relativity.
- The derived mass bounds highlight the limitations and specific applicability of massive graviton theories.
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