2003
DOI: 10.1070/sm2003v194n09abeh000767
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Exponential map in the generalized Dido problem

Abstract: We construct a new class of 1/4-BPS time dependent domain-wall solutions with null-like metric and dilaton in type II supergravities, which admit a null-like big bang singularity. Based on the domain-wall/QFT correspondence, these solutions are dual to 1/4-supersymmetric quantum field theories living on a boundary cosmological background with time dependent coupling constant and UV cutoff. In particular we evaluate the holographic c function for the 2-dimensional dual field theory living on the corresponding n… Show more

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Cited by 51 publications
(93 citation statements)
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References 32 publications
(33 reference statements)
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“…The general construction of elliptic coordinates was developed in [15,16,19], here they are adapted to the problem under consideration.…”
Section: Exponential Mappingmentioning
confidence: 99%
See 1 more Smart Citation
“…The general construction of elliptic coordinates was developed in [15,16,19], here they are adapted to the problem under consideration.…”
Section: Exponential Mappingmentioning
confidence: 99%
“…In the main Section 5 we obtain an explicit description of Maxwell strata corresponding to the group of discrete symmetries, and prove the upper bound on cut time. This approach was already successfully applied to the analysis of several invariant optimal control problems on Lie groups [15][16][17][18][19][20]. …”
mentioning
confidence: 99%
“…This techniques was already partially developed in the study of related optimal control problems (nilpotent sub-Riemannian problem with the growth vector (2, 3, 5) [13][14][15][16] and Euler's elastic problem [17,18]). The sub-Riemannian problem on SE(2) is the first problem in this series, where a complete solution was obtained (local and global optimality, cut time and cut locus, optimal synthesis).…”
Section: Resultsmentioning
confidence: 99%
“…, corresponding to discrete symmetries ε i . The following upper bound is the main result of work [9]: 13) where t(λ) = min(t 1 ε i (λ)) is the first Maxwell time corresponding to the group of symmetries G. We recall the explicit definition of the function t(λ) below in equations (2.20)-(2.24).…”
Section: Introductionmentioning
confidence: 99%
“…. , 8 as a frame of left-invariant vector fields on . Consider the left-invariant sub-Riemannian structure ( , Δ, ) defined by 1 , 2 as an orthonormal frame: Δ = span( 1 ( ), 2 ( )), ( , ) = .…”
Section: Letmentioning
confidence: 99%