1999
DOI: 10.1142/s0217751x99000415
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F Theory Vacua in Four Dimensions and Toric Threefolds

Abstract: We investigate D=4, N=1 F theory models realized by type IIB string compactification on toric threefolds. Massless spectra, gauge symmetries, phase transitions associated with divisor contractions and flops, and non-perturbative superpotentials are analyzed using elementary toric methods.

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Cited by 30 publications
(88 citation statements)
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“…In the higherdimensional fibration, the coefficients of the polynomials in p will become functions of the variables of the base B n -i. More precisely, (y, rr, i, v) become 9 Toric constructions of Calabi-Yau 4-folds have been discussed in [45,46,47,48,49].…”
Section: Description Of the Bundlementioning
confidence: 99%
See 1 more Smart Citation
“…In the higherdimensional fibration, the coefficients of the polynomials in p will become functions of the variables of the base B n -i. More precisely, (y, rr, i, v) become 9 Toric constructions of Calabi-Yau 4-folds have been discussed in [45,46,47,48,49].…”
Section: Description Of the Bundlementioning
confidence: 99%
“…This can be argued from considering a compactification on S 1 and comparison with M-theory, which leads to the following contribution of the hodge numbers of W4 to the four-dimensional fields [48] 24…”
Section: Non-perturbative Gauge Symmetries From Non-toric Basesmentioning
confidence: 99%
“…Again we refer to the literature for a more detailed analysis of the four-dimensional N = 1 spectrum and the translation to the heterotic side, see [183,[222][223][224] and [217] for a detailed derivation of the F-theory effective action in a dimensional reduction on X 4 . Upon a further compactification on T 2 heterotic/F-theory duality becomes heterotic/Type II duality in two dimensions which can alternatively be used for an discussion of the massless spectrum and effective action [151,225].…”
Section: Heterotic/f-theory Duality In Lower Dimensionsmentioning
confidence: 99%
“…18 of them are toric threefolds p n (1 n 18) and are completely classified [83,84,85,86]. They were studied in the context of Calabi-Yau fourfold compactifications over Fano threefolds [44,79]. In particular in [82], it was shown that for k 0Y XXXY 6 over B 3 k there exists a smooth Weierstrass model (having a section); B 3 k with k 0Y 1Y 2Y 3 correspond to the toric Fano three-folds p n with n 2Y 9Y 13Y 17.…”
Section: 1mentioning
confidence: 99%
“…One finds In the following we restrict to k 0Y 1Y 2Y 3 where one has h 21 0, [44,79], h 11 X 4 k 3 k, h 31 X 4 k c 6 À 8 À 3 k 28 3619 À k [44,79,25]. Now since we have a smooth Weierstrass model and thus expecting no unbroken gauge group, i.e.…”
Section: 1mentioning
confidence: 99%