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D-term Inflation and M-theory
High Energy Physics - Phenomenology · Submitted 2 Dec 1998
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We will show that such models still suffer from the other drawback of D-inflationary models, namely that Planckian field values are required to drive inflation.
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The abstract, sentence by sentence
Models of supersymmetric D-term inflation require a new mass scale near 10^{15-16} GeV in order to match the density perturbation spectrum observed by COBE. Attempts to obtain such a scale from the anomalous U(1) of string theories fail in most string models. However there is hope that models based on non-standard embeddings in M-theory can solve the discrepancy. We will show that such models still suffer from the other drawback of D-inflationary models, namely that Planckian field values are required to drive inflation. Thus it is hard to understand why the inflaton potential remains so flat without imposing stringent symmetries on the superpotential. We also examine a fascinating quasi-fixed point behavior for the gauge coupling of the anomalous U(1) in these extra-dimensional models, and show that either the presence of large numbers of fields in the 5-dimensional bulk or strongly suppressed U(1) gauge couplings is required in order to restore naturality to the inflationary potential.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Models of supersymmetric D-term inflation require a new mass scale near 10^{15-16} GeV in order to match the density perturbation spectrum observed by COBE. | background 1.00 | 0.07 | 0.04 | asserted 0.99 |
| s1 | Attempts to obtain such a scale from the anomalous U(1) of string theories fail in most string models. | background 0.89 | 0.07 | 0.03 | asserted 0.97 |
| s2 | However there is hope that models based on non-standard embeddings in M-theory can solve the discrepancy. | background 0.53 | 0.06 | 0.05 | hedged possibility 0.94 |
| s3 | We will show that such models still suffer from the other drawback of D-inflationary models, namely that Planckian field values are required to drive inflation. | result 0.75 | 0.76 | 0.60 | asserted 1.00 |
| s4 | Thus it is hard to understand why the inflaton potential remains so flat without imposing stringent symmetries on the superpotential. | interpretation 0.89 | 0.38 | 0.24 | asserted 0.56 |
| s5 | We also examine a fascinating quasi-fixed point behavior for the gauge coupling of the anomalous U(1) in these extra-dimensional models, and show that either the presence of large numbers of fields in the 5-dimensional bulk or strongly suppressed U(1) gauge couplings is required in order to restore naturality to the inflationary potential. | result 0.91 | 0.90 | 0.13 | asserted 1.00 |
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Original abstract
Models of supersymmetric D-term inflation require a new mass scale near 10^{15-16} GeV in order to match the density perturbation spectrum observed by COBE. Attempts to obtain such a scale from the anomalous U(1) of string theories fail in most string models. However there is hope that models based on non-standard embeddings in M-theory can solve the discrepancy. We will show that such models still suffer from the other drawback of D-inflationary models, namely that Planckian field values are required to drive inflation. Thus it is hard to understand why the inflaton potential remains so flat without imposing stringent symmetries on the superpotential. We also examine a fascinating quasi-fixed point behavior for the gauge coupling of the anomalous U(1) in these extra-dimensional models, and show that either the presence of large numbers of fields in the 5-dimensional bulk or strongly suppressed U(1) gauge couplings is required in order to restore naturality to the inflationary potential.
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