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Hint to Supersymmetry from GR Vacuum

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arxiv 2406.18402 v1 pith:INJCBI5S submitted 2024-06-26 hep-th gr-qchep-ph

classification hep-thgr-qchep-ph
keywords supersymmetryvacuumaxionfermionsgravitationalspin-anomalyinstantons
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

The $S$-matrix formulation of gravity suggests that the $\theta$-vacuum structure must not be sustained by the theory. We point out that, when applied to the vacuum of general relativity, this criterion hints to supersymmetry. The topological susceptibility of gravitational vacuum induced by Eguchi-Hanson instantons can be eliminated neither by spin-$1/2$ fermions nor by an axion coupled via them since such fermions do not provide instanton zero modes. Instead, the job is done by a spin-$3/2$ fermion, hence realizing a local supersymmetry. This scenario also necessitates the spontaneous breaking of supersymmetry and predicts the existence of axion of $R$-symmetry which gets mass exclusively from the gravitational instantons. The $R$-axion can be a viable dark matter candidate. Matching between the index and the anomaly imposes a constraint that spin-$1/2$ fermions should not contribute to the chiral gravitational anomaly.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. (Super)$\,$Gravity from Positivity

    hep-th 2025-07 conditional novelty 8.0 of 10

    Positivity of scattering amplitudes forces weakly coupled EFTs of a massive spin-3/2 particle to include gravity, and for charged states a gauged photon with g=2 and WGC-saturating charge.

  2. Emergent Dark Matter

    hep-ph 2025-11 conditional novelty 6.0 of 10

    Dark matter is modeled as the emergent massive in-medium state of a 3-form gauge field that otherwise behaves as dark energy.

  3. On Time-Evolution in Quantum Gravity

    hep-th 2025-10 conditional novelty 6.0 of 10

    The bulk Hamiltonian of BRST-quantized gravity is shown to be BRST-exact (H = Mpl∫{Q,iΠc0}) yet still produces the correct time evolution of bulk correlators of gauge-variant operators.

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