Abstract
As the theory is subject to a section condition, coordinates in double field theory do not represent physical points in an injective manner. We argue that a physical point should be rather one-to-one identified with a ‘gauge orbit’ in the coordinate space. The diffeomorphism symmetry then implies an invariance under arbitrary reparametrizations of the gauge orbits. Within this generalized sense of diffeomorphism, we show that a recently proposed tensorial transformation rule for finite coordinate transformations is actually (i) consistent with the standard exponential map, and further (ii) compatible with the full covariance of the ‘semi-covariant’ derivatives and curvatures after projectors are properly imposed.
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ArXiv ePrint: 1304.5946
On sabbatical leave of absence for calendar year 2013. (Jeong-Hyuck Park)
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Park, JH. Comments on double field theory and diffeomorphisms. J. High Energ. Phys. 2013, 98 (2013). https://doi.org/10.1007/JHEP06(2013)098
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DOI: https://doi.org/10.1007/JHEP06(2013)098