2020
DOI: 10.1103/physrevlett.124.211603
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Vacua with Small Flux Superpotential

Abstract: We introduce a method for finding flux vacua of type IIB string theory in which the flux superpotential is exponentially small and at the same time one or more complex structure moduli are stabilized exponentially near to conifold points.

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Cited by 125 publications
(292 citation statements)
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“…Having more fields at high energies that break the scaling symmetries means including more spurions in the low-energy theory, potentially undermining the conclusions drawn above about the form dictated by scaling for K and W. 47 To see what is involved consider a spurion, W 0 , representing an expectation for the field G 3 itself. When W 0 = 0 the dilaton remains a massless Goldstone boson (see [176] for an explicit example) while when the spurion W 0 is non-zero, one of the scaling symmetries is explicitly broken and the dilaton becomes massive. This spurion scales as W 0 → w W 0 , as does G 3 .…”
Section: Other Fields and Spurionsmentioning
confidence: 99%
“…Having more fields at high energies that break the scaling symmetries means including more spurions in the low-energy theory, potentially undermining the conclusions drawn above about the form dictated by scaling for K and W. 47 To see what is involved consider a spurion, W 0 , representing an expectation for the field G 3 itself. When W 0 = 0 the dilaton remains a massless Goldstone boson (see [176] for an explicit example) while when the spurion W 0 is non-zero, one of the scaling symmetries is explicitly broken and the dilaton becomes massive. This spurion scales as W 0 → w W 0 , as does G 3 .…”
Section: Other Fields and Spurionsmentioning
confidence: 99%
“…However, a full understanding of this question requires detailed (numerical) studies of the distributions of flux vacua which is well beyond the scope of the present work. For estimates of the number of vacua as a function of the flux superpotential and the string coupling see [40][41][42][43][44].…”
Section: Jhep10(2020)015mentioning
confidence: 99%
“…Given that LVS models can be realised for natural values of the vacuum expectation value of the flux superpotential, |W 0 | ∼ O(1 − 10), while KKLT models can be constructed only via tuning |W 0 | to exponentially small values (similar considerations about tuning of the underlying parameters apply also to perturbatively stabilised vacua), we tend to conclude that the distribution of the scale of supersymmetry breaking seems to be logarithmic. However, more detailed studies are needed in order to find a precise definite answer to this important question (see [40][41][42][43][44] for initial studies on the determination of the number of vacua as a function of |W 0 | and g s ).…”
Section: Jhep10(2020)015mentioning
confidence: 99%
“…see e.g. [26,45,[53][54][55][56][57][58][59][60][61]. This is an elliptic fibration with h 1,1 = 2, h 2,1 = 272, hence χ = −540, with a typical fiber in the configuration E 6 ∈ P (1,2,3) [6].…”
Section: 2mentioning
confidence: 99%