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Towards Finite Quantum Field Theory in Non-Commutative Geometry

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arxiv hep-th/9505175 v1 pith:WHJ7OBAI submitted 1995-05-29 hep-th

Towards Finite Quantum Field Theory in Non-Commutative Geometry

classification hep-th
keywords fieldfinitespheretheoryapproachautomaticallydescribeexplicitely
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We describe the self-interacting scalar field on the truncated sphere and we perform the quantization using the functional (path) integral approach. The theory posseses a full symmetry with respect to the isometries of the sphere. We explicitely show that the model is finite and the UV-regularization automatically takes place.

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Cited by 4 Pith papers

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

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    hep-th 2026-07 conditional novelty 7.0

    Fuzzy-sphere horizon partons form LLL states under a Berry monopole and, after link condensation locks the horizon gauge field to the exterior Maxwell field, generate a physical membrane current with quantum correctio...

  2. Quantum Horizon and Quantum Membrane Paradigm from Black Hole Quantum Mechanics

    hep-th 2026-07 conditional novelty 7.0

    Horizon partons on the fuzzy sphere form lowest-Landau-level states under an intrinsic Berry monopole, generating Ohmic, Hall and polarization currents that a link-field condensate locks to the bulk Maxwell field, yie...

  3. Quantum simulation of gauge theories on dynamical spacetimes via Floquet-induced matrix models

    quant-ph 2026-07 conditional novelty 7.0

    Ensemble-averaged Floquet fidelities of Haar-random states reproduce Euclidean Yang-Mills matrix path-integral weights at leading order, enabling lattice-free quantum simulation of gauge fields on dynamical geometries.

  4. 3d Conformal Field Theories via Fuzzy Sphere Algebra

    cond-mat.str-el 2026-02 conditional novelty 6.0

    The fuzzy-sphere density-mode algebra is a genuine Lie algebra, but a direct density-mode realization of the 3d conformal algebra so(3,2) exists only for the two-electron system.