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Lorentzian and signature changing branes

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arxiv 0705.3380 v1 pith:KREZQC7F submitted 2007-05-23 hep-th gr-qc

classification hep-thgr-qc
keywords signaturechangebranebraneshypersurfaceshellsdescriptionallows
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

General hypersurface layers are considered in order to describe brane-worlds and shell cosmologies. No restriction is placed on the causal character of the hypersurface which may thus have internal changes of signature. Strengthening the results in our previous letter [1], we confirm that a good, regular and consistent description of signature change is achieved in these brane/shells scenarios, while keeping the hypersurface and the bulk completely regular. Our formalism allows for a unified description of the traditional timelike branes/shells together with the signature-changing, or pure null, ones. This allows for a detailed comparison of the results in both situations. An application to the case of hypersurface layers in static bulks is presented, leading to the general Robertson-Walker geometry on the layer --with a possible signature change. Explicit examples on anti de Sitter bulks are then studied. The permitted behaviours in different settings ($Z_{2}$-mirror branes, asymmetric shells, signature-changing branes) are analysed in detail. We show in particular that (i) in asymmetric shells there is an upper bound for the energy density, and (ii) that the energy density within the brane vanishes when approaching a change of signature. The description of a signature change as a `singularity' seen from within the brane is considered. We also find new relations between the fundamental constants in the brane/shell, its tension, and the cosmological and gravitational constants of the bulk, independently of the existence or not of a change of signature.

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  1. Inflation from Covariant Signature Change: A Geometric Mechanism

    gr-qc 2026-06 unverdicted novelty 5.0 of 10

    A covariant signature-change layer between a Euclidean cap and a Lorentzian universe acts as a geometric, inflaton-free fluid that accelerates expansion while the interpolator slope exceeds a curvature-dependent threshold.

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