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Transitions in the Web of Heterotic Vacua
High Energy Physics - Theory · Submitted 14 Dec 2010
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We demonstrate how such transitions can change important properties of the effective theory, including the gauge symmetry and the massless spectrum.
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The abstract, sentence by sentence
We analyze transitions between heterotic vacua with distinct gauge bundles using two complementary methods - the effective four-dimensional field theory and the corresponding geometry. From the viewpoint of effective field theory, such transitions occur between flat directions of the potential energy associated with heterotic stability walls. Geometrically, this branch structure corresponds to smooth deformations of the gauge bundle coupled to the chamber structure of K\"ahler moduli space. We demonstrate how such transitions can change important properties of the effective theory, including the gauge symmetry and the massless spectrum. Geometrically, this study is divided into deformations of the vector bundle which preserve the rank of the gauge bundle and those which change the rank. In the latter case, our results provide explicit solutions to a class of Li-Yau type deformation problems. Finally, we use the framework of stability walls and their effective theory to study Donaldson-Thomas invariants on Calabi-Yau threefolds.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We analyze transitions between heterotic vacua with distinct gauge bundles using two complementary methods - the effective four-dimensional field theory and the corresponding geometry. | contribution 0.74 | 0.94 | 0.09 | asserted 0.99 |
| s1 | From the viewpoint of effective field theory, such transitions occur between flat directions of the potential energy associated with heterotic stability walls. | result 0.41 | 0.41 | 0.10 | asserted 1.00 |
| s2 | Geometrically, this branch structure corresponds to smooth deformations of the gauge bundle coupled to the chamber structure of K\"ahler moduli space. | interpretation 0.60 | 0.44 | 0.11 | asserted 1.00 |
| s3 | We demonstrate how such transitions can change important properties of the effective theory, including the gauge symmetry and the massless spectrum. | result 0.83 | 0.91 | 0.33 | asserted 0.97 |
| s4 | Geometrically, this study is divided into deformations of the vector bundle which preserve the rank of the gauge bundle and those which change the rank. | method 0.75 | 0.71 | 0.07 | asserted 0.99 |
| s5 | In the latter case, our results provide explicit solutions to a class of Li-Yau type deformation problems. | result 0.84 | 0.90 | 0.10 | asserted 1.00 |
| s6 | Finally, we use the framework of stability walls and their effective theory to study Donaldson-Thomas invariants on Calabi-Yau threefolds. | contribution 0.97 | 0.92 | 0.17 | asserted 1.00 |
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The paper
Original abstract
We analyze transitions between heterotic vacua with distinct gauge bundles using two complementary methods - the effective four-dimensional field theory and the corresponding geometry. From the viewpoint of effective field theory, such transitions occur between flat directions of the potential energy associated with heterotic stability walls. Geometrically, this branch structure corresponds to smooth deformations of the gauge bundle coupled to the chamber structure of K\"ahler moduli space. We demonstrate how such transitions can change important properties of the effective theory, including the gauge symmetry and the massless spectrum. Geometrically, this study is divided into deformations of the vector bundle which preserve the rank of the gauge bundle and those which change the rank. In the latter case, our results provide explicit solutions to a class of Li-Yau type deformation problems. Finally, we use the framework of stability walls and their effective theory to study Donaldson-Thomas invariants on Calabi-Yau threefolds.
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References
How the literature uses it
22 arXiv papers cite this in 59 sentences
Papers citing it · 43 sentences without a confident label
Uses its method or tool 2 papers
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It is important to note that, instead of adopting the standard embedding, we shall loosely adopt the setting outlined in [ref] , in which moduli fixing is achieved by making a judicious choice of the gauge bundle and non-perturbative superpotentials coming from gaugino condensates and string instantons.
Natural Inflation from Near Alignment in Heterotic String Theory · The Model · 0.96
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Of the three approaches to complex structure stabilization illustrated in Section [ref], here we use the effective field theory [ref] and geometric methods associated with the bundle double_ext.
The Atiyah Class and Complex Structure Stabilization in Heterotic Calabi-Yau Compactifications · “Jumping" Tri-linear Couplings · 0.91
Uses its data or values 1 paper
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In Ref. [ref] , the DT invariant has been obtained from this as DT(X,c = (2, (0,0), (-4,6), 0 ) ; ω= t^1 J_1 + t^2 J_2 ) = -10 , if $4< t^2/t^1 < ∞$ , 0 , if $0<t^2/t^1 ≤4$ , which is seen to jump when one crosses the stability wall of [ref].
Quiver Structure of Heterotic Moduli · A Rank-2 Example: $SU(2) →S[U(1) ×U(1)]$ · 0.95
Cites it as support 3 papers
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However, as shown in [ref] , this new bundle is actually isomorphic to the above, that is
Hidden Sectors from Multiple Line Bundles for the $B-L$ MSSM · Extension Bundle · 0.97
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As shown in [ref] , one can turn on this combination of VEVs while still having the superpotential and its derivative vanish – that is, the effective theory satisfies the F-flatness requirement.
The strongly coupled $E_8\times E_8$ heterotic string: Geometry $\&$ Phenomenology · Extension Bundle · 0.97
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As it turns out this simple construction of $SU(2)$ bundles[This class of bundles can be used to make manifest the 4-dimensional D-terms related to slope stability [ref] .] has been shown [ref] to fix nearly all the complex structure moduli of $X$!
TASI Lectures on Geometric Tools for String Compactifications · Manifolds, Bundles and Moduli Problems · 0.97
Cites it as background 5 papers
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Previous work [ref] - [ref] investigated the constraints arising from $g^ab̅F_ab̅=0$, the slope-stability condition [ref] on $V$, and the conditions this places on the combined Kähler and vector bundle moduli spaces.
The Atiyah Class and Complex Structure Stabilization in Heterotic Calabi-Yau Compactifications · Introduction · 0.86
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In the latter case, such loci can lead to complicated branch structure in the vacuum space of the theory in which many different bundles over the same $X$ are connected [ref] .
New Evidence for (0,2) Target Space Duality · Introduction · 0.80
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Such F-term obstructions must be explored on a case-by-case basis (see [ref] for further discussions).
Heterotic Line Bundle Standard Models · Connecting different splitting types · 0.82
What it cites · 64 sentences without a confident label
Cites as background 19 papers
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In Section [ref], we give a brief review of Kähler cone substructure and stability walls, from both a geometric and field theoretic standpoint [ref] .
Stability Walls in Heterotic Theories · Introduction · 1.00
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In Section [ref], we give a brief review of Kähler cone substructure and stability walls, from both a geometric and field theoretic standpoint [ref] .
Kahler Cone Substructure · Introduction · 1.00
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In Section [ref], we give a brief review of Kähler cone substructure and stability walls, from both a geometric and field theoretic standpoint [ref] .
Yukawa Textures From Heterotic Stability Walls · Introduction · 1.00
Discussion
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