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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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arXiv IDhep-ph/9812234 (version 1)
Pith IDBFGVKZ77, Pith's permanent record of this paper and its review
CitationChristopher Kolda, David H. Lyth. "D-term Inflation and M-theory." arXiv:hep-ph/9812234 (1998). https://pith.science/paper/BFGVKZ77
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 5,009 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.89 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.50 · compares with prior results 0.69 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

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

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
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

What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from proof or derivation 0.78.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
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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