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Codimension-Three Bundle Singularities in F-Theory
High Energy Physics - Theory · Submitted 27 Sep 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim These degenerations result in new four-dimensional infrared physics characterized by light solitonic states whose origin is explained in the dual F-theory model.
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The abstract, sentence by sentence
We study new nonperturbative phenomena in N=1 heterotic string vacua corresponding to pointlike bundle singularities in codimension three. These degenerations result in new four-dimensional infrared physics characterized by light solitonic states whose origin is explained in the dual F-theory model. We also show that such phenomena appear generically in $E_7 \to E_6$ Higgsing and describe in detail the corresponding bundle transition.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study new nonperturbative phenomena in N=1 heterotic string vacua corresponding to pointlike bundle singularities in codimension three. | contribution 1.00 | 0.90 | 0.23 | asserted 0.98 |
| s1 | These degenerations result in new four-dimensional infrared physics characterized by light solitonic states whose origin is explained in the dual F-theory model. | result 0.81 | 0.72 | 0.38 | asserted 1.00 |
| s2 | We also show that such phenomena appear generically in $E_7 \to E_6$ Higgsing and describe in detail the corresponding bundle transition. | result 0.52 | 0.93 | 0.26 | asserted 1.00 |
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The paper
Original abstract
We study new nonperturbative phenomena in N=1 heterotic string vacua corresponding to pointlike bundle singularities in codimension three. These degenerations result in new four-dimensional infrared physics characterized by light solitonic states whose origin is explained in the dual F-theory model. We also show that such phenomena appear generically in $E_7 \to E_6$ Higgsing and describe in detail the corresponding bundle transition.
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References
How the literature uses it
28 arXiv papers cite this in 42 sentences
Papers citing it · 35 sentences without a confident label
Compares with it 1 paper
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Some of these results in this section resemble those obtained from the spectral construction of stable sheaves on elliptic fibrations (e.g. see [ref] ), as well as results obtained by Yoshioka, where he assumes the existence of a section for the fibration (see [ref] ).
Stability and Fourier-Mukai transforms on elliptic fibrations · Application 2: pure codimension-1 sheaves · 0.96
Cites it as support 1 paper
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If the Weierstrass coefficients $f$ and $g$ have multiplicities at $P_μ$ which exceed $4$ for $f$ and $6$ for $g$, then there is no desingularization of the Weierstrass model which is flat [ref] , which means that there would be tensionless strings in the low-energy theory.
Box Graphs and Singular Fibers · Local models for fibers in codimension three · 0.96
Cites it as background 4 papers
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The physics of this a non-flat fibration has been discussed in [ref] .
Chiral Four-Dimensional F-Theory Compactifications With SU(5) and Multiple U(1)-Factors · Yukawa Couplings: Codimension Three · 0.92
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In the context of F-theory, such fibrations have been systematically studied in [ref] for Kodaira fibers, with examples in codimension two and three appearing in [ref] .
Fibers add Flavor, Part I: Classification of 5d SCFTs, Flavor Symmetries and BPS States · Introduction · 0.94
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Many F-theory geometries contain $(4, 6)$ (or higher) singularities in the elliptic fibration over codimension-three loci in the base [ref] ; these are often associated with non-flat fibers in the resolution [ref] .
Chiral matter multiplicities and resolution-independent structure in 4D F-theory models · Codimension-three $(4, 6)$ loci · 0.98
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