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Type: Preprint
Gauge from holography
Abstract:
In a spacetime divided into two regions U1 and U2 by a hypersurface \Sigma, a perturbation of the field in U1 is coupled to perturbations in U2 by means of the first-order holographic imprint that it leaves on \Sigma. The linearized glueing field equation constrains perturbations on the two sides of a dividing hypersurface. This linear operator may have a nontrivial null space; a nontrivial perturbation of the field leaving a holographic imprint on a dividing hypersurface which does not affect perturbations on the other side should be considered physically irrelevant. This condition, together with a locality requirement, leads to the notion of gauge equivalence in first-order Lagrangian field theory.
In a spacetime divided into two regions U1 and U2 by a hypersurface \Sigma, a perturbation of the field in U1 is coupled to perturbations in U2 by means of the first-order holographic imprint that it leaves on \Sigma. The linearized glueing field equation constrains perturbations on the two sides of a dividing hypersurface. This linear operator may have a nontrivial null space; a nontrivial perturbation of the field leaving a holographic imprint on a dividing hypersurface which does not affect perturbations on the other side should be considered physically irrelevant. This condition, together with a locality requirement, leads to the notion of gauge equivalence in first-order Lagrangian field theory.
MSC: 70S15, 83C30, 81T13, 70S05
Year Preprint: 2017
Report Number: UNAM-CCM-2017-3
arXiv: arXiv:1704.07959 [gr-qc]



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