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Fermions in Loop Quantum Gravity and Resolution of Doubling Problem

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arxiv 2212.00933 v1 pith:LN7AS7J4 submitted 2022-12-02 gr-qc hep-lathep-th

classification gr-qchep-lathep-th
keywords quantumfermiongravitylooppropagatorstatesuperpositiondoubling
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The fermion propagator is derived in detail from the model of fermion coupled to loop quantum gravity. As an ingredient of the propagator, the vacuum state is defined as the ground state of some effective fermion Hamiltonian under the background geometry given by a coherent state resembling the classical Minkowski spacetime. Moreover, as a critical feature of loop quantum gravity, the superposition over graphs is employed to define the vacuum state. It turns out that the graph superposition leads to the propagator being the average of the propagators of the lattice field theory over various graphs so that all fermion doubler modes are suppressed in the propagator. This resolves the doubling problem in loop quantum gravity. Our result suggests that the superposition nature of quantum geometry should, on the one hand, resolve the tension between fermion and the fundamental discreteness and, on the other hand, relate to the continuum limit of quantum gravity.

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Cited by 2 Pith papers

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

  1. An inquiry on the Absence of Fermion Doubling and why the Nielsen-Ninomiya Theorem Does Not Apply to Nonlocal Quantum Field Theory

    hep-th 2026-07 accept novelty 5.0 of 10

    A continuum nonlocal Dirac operator multiplied by an invertible zero-free entire function has exactly the same kernel and finite-momentum zero set as the ordinary Dirac operator, so fermion doubling is absent.

  2. Testing Einstein Maxwell Power-Yang-Mills Hair via Black Hole Photon Rings

    gr-qc 2025-01 reject novelty 3.0 of 10

    For the p=1/2 Einstein-Maxwell power-Yang-Mills black hole, increasing the hair parameter Q_YM shrinks the horizon, photon sphere, ISCO, shadow, and photon ring, an effect equivalent to a mass shift in Reissner-Nordström.

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