1991
DOI: 10.1016/0370-2693(91)91831-f
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From trivial to non-trivial conformal string backgrounds via O(d, d) transformations

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Cited by 108 publications
(99 citation statements)
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“…the curvature and dilaton have become singular at some fixed proper time. There have been a number of suggested ways to tackle the singularity problem, considering also anisotropic [25,26] and inhomogeneous [27,28] backgrounds, or the presence of a non-local dilaton potential [2]. However, if we confine our attention to homogeneous and isotropic metrics, and to a local potential, one of the most promising approaches to the graceful exit problem [29] suggests that the curvature singularities may be cured by adding higher-order corrections to the string effective action (see for instance [30,31,32,3,4,6]).…”
Section: Introductionmentioning
confidence: 99%
“…the curvature and dilaton have become singular at some fixed proper time. There have been a number of suggested ways to tackle the singularity problem, considering also anisotropic [25,26] and inhomogeneous [27,28] backgrounds, or the presence of a non-local dilaton potential [2]. However, if we confine our attention to homogeneous and isotropic metrics, and to a local potential, one of the most promising approaches to the graceful exit problem [29] suggests that the curvature singularities may be cured by adding higher-order corrections to the string effective action (see for instance [30,31,32,3,4,6]).…”
Section: Introductionmentioning
confidence: 99%
“…[2]). For example, this symmetry has been employed to generate curved backgrounds with a time-dependent tensor potential from flat solutions [10] and homogeneous cosmologies [11]. On the other hand the presence of an SL(2,R) symmetry [12] in the NS-NS sector of the theory can been used to generate a time-dependent field-strength [13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…I have included a general dilaton potential, V (φ), and the possible phenomenological contribution of other sources, represented generically by T ν µ . By setting V = 0 and T µν = 0 we find for the system (9.7) the particular exact (anisotropic) solution [7] (with non-trivial torsion H µνα = 0)…”
Section: Possible Origin Of the Cmb Radiationmentioning
confidence: 99%
“…(9.8) Such solution can also be obtained by "inverting" and appropriately "boosting" (through scale factor duality and O(2, 2) transformations) the globally flat metric [7] …”
Section: Possible Origin Of the Cmb Radiationmentioning
confidence: 99%
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