2022
DOI: 10.48550/arxiv.2201.01679
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Geometric Flow of Bubbles

Davide De Biasio,
Dieter Lust

Abstract: In this work we derive a class of geometric flow equations for metric-scalar systems. Thereafter, we construct them from some general string frame action by performing volume-preserving fields variations and writing down the associated gradient flow equations. Then, we consider some specific realisations of the above procedure, applying the flow equations to non-trivial scalar bubble and metric bubble solutions, studying the subsequent flow behaviour.

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Cited by 3 publications
(34 citation statements)
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“…s-structure) of a cotangent Lorentz bundle M = T * V, dim V = 4, as in [12,13,41]. Star product R-flux deformations of fundamental geometry s-objects (27), determined by nonassociative geometric data s g ⋆ (τ ), s D ⋆ (τ ) , are performed following Convention 2 (26) with κ-linear parametric decompositions when ⋆ ǧ[0] αsβs (τ ) = ⋆ g αsβs (τ ) = g αsβs (τ ). Geometric flows on a parameter τ are described in [0]-approximation (zero power on κ) by flows of some canonical data ( s g(τ ), s D(τ )), star product flows ⋆ s (τ ), determined by s-adapted frames e is (τ ) in (19), and flows of volume elements…”
Section: Nonassociative Generalizations Of Perelman's F-and W-functio...mentioning
confidence: 99%
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“…s-structure) of a cotangent Lorentz bundle M = T * V, dim V = 4, as in [12,13,41]. Star product R-flux deformations of fundamental geometry s-objects (27), determined by nonassociative geometric data s g ⋆ (τ ), s D ⋆ (τ ) , are performed following Convention 2 (26) with κ-linear parametric decompositions when ⋆ ǧ[0] αsβs (τ ) = ⋆ g αsβs (τ ) = g αsβs (τ ). Geometric flows on a parameter τ are described in [0]-approximation (zero power on κ) by flows of some canonical data ( s g(τ ), s D(τ )), star product flows ⋆ s (τ ), determined by s-adapted frames e is (τ ) in (19), and flows of volume elements…”
Section: Nonassociative Generalizations Of Perelman's F-and W-functio...mentioning
confidence: 99%
“…We omit such technical details in this work because they can be derived in abstract form following geometric principles and the Convention 2 (26). For recent applications in high energy physics, we cite [23,24,25,26,27] where the normalizing function is postulated as a dilaton field and associative and commutative versions of metric-dilaton Ricci flows are investigated. Certain geometric flow equations can be also motivated as star product R-flux deformations of a two-dimensional sigma model with beta functions and dilaton field (see equations ( 79) and (80) in [23]).…”
Section: A S-adapted Variational Procedures For Deriving Nonassociati...mentioning
confidence: 99%
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