2002
DOI: 10.1016/s0550-3213(02)00434-0
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Modular-invariant anomalous U(1) breaking

Abstract: We describe the effective supergravity theory present below the scale of spontaneous gauge symmetry breaking due to an anomalous U (1), obtained by integrating out tree-level interactions of massive modes. A simple case is examined in some detail. We find that the effective theory can be expressed in the linear multiplet formulation, with some interesting consequences. Among them, the modified linearity conditions lead to new interactions not present in the theory without an anomalous U (1). These additional i… Show more

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Cited by 12 publications
(16 citation statements)
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“…Then these VEVs would be much larger since typically (Λ X /m pl ) ∼ 1/10 and an electroweak-scale µ term would require an operator of rather large dimension. For anomalous U (1) breaking we expect the combination of fields cancelling the Fayet-Illiopoulos term to preserve modular invariance [29]. Therefore the canonically normalized effective µ term is given by…”
Section: A First Approach: Weakly Coupled Heterotic String Theorymentioning
confidence: 99%
“…Then these VEVs would be much larger since typically (Λ X /m pl ) ∼ 1/10 and an electroweak-scale µ term would require an operator of rather large dimension. For anomalous U (1) breaking we expect the combination of fields cancelling the Fayet-Illiopoulos term to preserve modular invariance [29]. Therefore the canonically normalized effective µ term is given by…”
Section: A First Approach: Weakly Coupled Heterotic String Theorymentioning
confidence: 99%
“…Note that we have only considered the case with X-Higgses charged solely under U(1) X . The analogous vacuum selection which occurs for the more general case of X-Higgses charged under several factors of the gauge group will be considered elsewhere [8].…”
Section: Effective Scalar Potentialmentioning
confidence: 96%
“…MKG has found ways to: consistently fix to unitary gauge (not an easy task with dynamical string moduli); preserve manifest target-space modular invariance; effectively include tree-level exchange of heavy multiplets in the general case of many fields and U(1)'s. The machinery is forthcoming [8].…”
Section: Scopementioning
confidence: 99%
“…In Section 4.1 we illustrate the procedure for integrating out the massive vector supermultiplet while preserving manifest local supersymmetry and T-duality in the lower energy effective theory using a toy model 156 with just one broken gauge symmetry, U (1) X , and just one complex scalar vev; in Section 4.2 we include hidden sector gaugino condensation in this toy model. Since the linear multiplet formalism for the dilaton is by far better suited to addressing these questions, we will use it in these two sections, and impose further that the modified linearity condition (42) remain true in the effective theory below the U (1) X breaking scale.…”
Section: Inclusion Of Anomalous U(1)'smentioning
confidence: 99%