2011
DOI: 10.1007/jhep01(2011)012
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Axions in the landscape and string theory

Abstract: While axions seem ubiquitous in critical string theories, whether they might survive in any string theoretic description of nature is a difficult question. With some mild assumptions, one can frame the issues in the case that there is an approximate supersymmetry below the underlying string scale. The problem of axions is then closely tied to the question of how moduli are fixed. We consider, from this viewpoint, the possibility that supersymmetry is broken at an intermediate scale, as in "gravity mediation", … Show more

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Cited by 29 publications
(31 citation statements)
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References 29 publications
(62 reference statements)
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“…One explanation is that the QCD axion arises from the string theory axions, and is subject to the other moduli stabilization mechanism [33]. There appears a small number in the moduli stabilization, namely the ratio of the gravitino mass to the Planck scale, which could be extremely small if the SUSY persists to low-energy scales.…”
Section: Dark Mattermentioning
confidence: 99%
“…One explanation is that the QCD axion arises from the string theory axions, and is subject to the other moduli stabilization mechanism [33]. There appears a small number in the moduli stabilization, namely the ratio of the gravitino mass to the Planck scale, which could be extremely small if the SUSY persists to low-energy scales.…”
Section: Dark Mattermentioning
confidence: 99%
“…, this periodicity implies that, for large s, in the superpotential the axion appears as e −A . Solving the strong CP problem then requires suppressing only a small number of possible terms [28,29]. As always, in string theory, one has to understand stabilization of moduli.…”
Section: Large Field Solutions Of the Strong Cp Problemmentioning
confidence: 99%
“…The size of terms in the effective action associated with these fields is controlled by the 2π periodicity of the axions. If we denote the full chiral axion superfield by A = s + ia, this periodicity implies that, for large s, in the superpotential the axion appears as e −nA for integer n. In constructing models which include supersymmetry breaking, solving the strong CP problem requires suppressing only a small number of possible terms [38,39].…”
Section: Small Field and Large Field Solutions To The Strong Cp Problemmentioning
confidence: 99%