1987
DOI: 10.1143/ptp.77.773
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Vacuum Energies of String Compactified on Torus

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Cited by 21 publications
(19 citation statements)
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“…Combining the equations (5.13) and (5.14), we finally find 15) which is nothing but the third of the CDJ gauge transformation (3.4).…”
Section: Lie Algebroid Gauged Sigma Modelsmentioning
confidence: 88%
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“…Combining the equations (5.13) and (5.14), we finally find 15) which is nothing but the third of the CDJ gauge transformation (3.4).…”
Section: Lie Algebroid Gauged Sigma Modelsmentioning
confidence: 88%
“…T-dualisability is a rare property of non-linear sigma-models and it is not known what necessary conditions must be imposed on a target space metric G, and closed 3-form field H, such that the corresponding sigma-model has a T-dual with ( G, H). On the other hand, several sufficient conditions are known, giving various T-dualities like the Abelian one [9,15] or non-Abelian one [7,6,5,1], both in turn included as special cases of Poisson-Lie T-duality [11,10]. Chatzistavrakidis, Deser and Jonke (CDJ in what follows) recently proposed a new set of sufficient conditions which, they claimed, would give rise to new examples of T-dual pairs [3].…”
Section: Introductionmentioning
confidence: 99%
“…These coordinates are invariant under T -duality, and are sometimes called spectator fields or external coordinates. 2 The position of the indices a, b is changed due to the exchange Ta ↔ T a .…”
Section: Dressing Cosetsmentioning
confidence: 99%
“…To perform a PL T -duality with respect to the isometry group O(4), we need the general framework (see e.g., [11]). However, S 3 is isomorphic to SU(2), and we can perform the standard PL T -duality with respect to this SU (2). Other examples are the PL T -duality of coset spaces, AdS2 and S 2 .…”
Section: Dressing Cosetsmentioning
confidence: 99%
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