2001
DOI: 10.1016/s0550-3213(01)00202-4
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The dilaton potential from

Abstract: Recent understanding of N = 1 * supersymmetric theory (mass deformed N = 4) has made it possible to find an exact superpotential which encodes the properties of the different phases of the theory. We consider this superpotential as an illustrative example for the source of a nontrivial scalar potential for the string theory dilaton and study its properties. The superpotential is characterized by the rank of the corresponding gauge group (N ) and integers p, q, k labelling the different massive phases of the th… Show more

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Cited by 5 publications
(3 citation statements)
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“…(26) of interest to us here, would be, for instance, that of a 'run away' pre big bang type [37] dilaton potential, in the range where the dilaton slowly approaches a constant value asymptotically and with a decaying trend ∂V (Φ)/∂Φ < 0. Interestingly, this situation characterises N=1 globally supersymmetric theories that can be embedded in a supergravity/superstring framework [38]. 10 It is then straightforward to see that, under the above conditions, the higher order terms in (65) have either vanishing contributions to the equations of motion, or are subleading, for sufficiently smallḃ ≪ M 2 Pl , as required in the approach of [2], for our cosmic background solutions in a FLRW space time.…”
Section: Discussionmentioning
confidence: 95%
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“…(26) of interest to us here, would be, for instance, that of a 'run away' pre big bang type [37] dilaton potential, in the range where the dilaton slowly approaches a constant value asymptotically and with a decaying trend ∂V (Φ)/∂Φ < 0. Interestingly, this situation characterises N=1 globally supersymmetric theories that can be embedded in a supergravity/superstring framework [38]. 10 It is then straightforward to see that, under the above conditions, the higher order terms in (65) have either vanishing contributions to the equations of motion, or are subleading, for sufficiently smallḃ ≪ M 2 Pl , as required in the approach of [2], for our cosmic background solutions in a FLRW space time.…”
Section: Discussionmentioning
confidence: 95%
“…Thus, we see from (39) that the negative value of the ρ gCS is essential for the consistency of the approach, since it is only then that the energy conservation of the total stress energy tensor (13) leads to consistent results, given the positivity of ρ b . From (38) and (39) we then obtain…”
Section: Gravitational-anomaly-induced Inflation Through Running Vacuummentioning
confidence: 99%
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