2006
DOI: 10.1007/s00220-005-1501-8
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Nonassociative Tori and Applications to T-Duality

Abstract: Abstract. In this paper, we initiate the study of C * -algebras A endowed with a twisted action of a locally compact Abelian Lie group G, and we construct a twisted crossed product A⋊G, which is in general a nonassociative, noncommutative, algebra. The duality properties of this twisted crossed product algebra are studied in detail, and are applied to T-duality in Type II string theory to obtain the T-dual of a general principal torus bundle with general H-flux, which we will argue to be a bundle of noncommuta… Show more

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Cited by 116 publications
(235 citation statements)
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“…Then the Buscher rules [34] allow one to T-dualize along either the y or z directions, resulting in metric flux ω y xz or ω z xy , or T-dualize in y and z, resulting in Q yz x , but it is not obvious how to perform the third T-duality here to get R xyz ; our trivialization broke the third isometry, and the Buscher rules no longer apply. Indeed, there are general arguments that any tendimensional origin for R-flux cannot even have a local description [6,35]. So it is very much of interest to ask which configurations can be constructed from ten dimensions.…”
Section: Summary and Puzzlesmentioning
confidence: 99%
“…Then the Buscher rules [34] allow one to T-dualize along either the y or z directions, resulting in metric flux ω y xz or ω z xy , or T-dualize in y and z, resulting in Q yz x , but it is not obvious how to perform the third T-duality here to get R xyz ; our trivialization broke the third isometry, and the Buscher rules no longer apply. Indeed, there are general arguments that any tendimensional origin for R-flux cannot even have a local description [6,35]. So it is very much of interest to ask which configurations can be constructed from ten dimensions.…”
Section: Summary and Puzzlesmentioning
confidence: 99%
“…In [13], [14] the case of principle torus bundles was discussed. Dimensional reduction of H on the T d fibres gives forms H 3 , H 2 , H 1 , H 0 where H p is a p-form on the base.…”
Section: Introductionmentioning
confidence: 99%
“…The cochain twist deformation quantization techniques originally developed by [25] were motivated by the search for a systematic way to generalize notions of differential geometry to such non-geometric backgrounds, and in particular to construct nonassociative deformations of field theory and ultimately gravity (see also [3]); this approach is different in spirit to the nonassociative twist deformation of the geometric f-flux frame considered in [18], which does not seem to be of relevance for non-geometric string theory, nor does it agree with the string theory inspired nonassociative torus bundles of [14,19] which reproduce the classical limit only up to Morita equivalence. Physically consistent models with novel properties in the context of quantum mechanics were constructed in [25] using this formalism, and of Euclidean scalar quantum field theory in [23].…”
Section: G E Barnes a Schenkel And R J Szabomentioning
confidence: 99%