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Heterotic compactifications with principal bundles for general groups and general levels
High Energy Physics - Theory · Submitted 26 Jan 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This technology gives us a very general approach to handling heterotic compactifications with arbitrary principal bundles.
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The abstract, sentence by sentence
We examine to what extent heterotic string worldsheets can describe arbitrary E8xE8 gauge fields. The traditional construction of heterotic strings builds each E8 via a Spin(16)/Z2 subgroup, typically realized as a current algebra by left-moving fermions, and as a result, only E8 gauge fields reducible to Spin(16)/Z2 gauge fields are directly realizable in standard constructions. However, there exist perturbatively consistent E8 gauge fields which can not be reduced to Spin(16)/Z2, and so cannot be described within standard heterotic worldsheet constructions. A natural question to then ask is whether there exists any (0,2) SCFT that can describe such E8 gauge fields. To answer this question, we first show how each ten-dimensional E8 partition function can be built up using other subgroups than Spin(16)/Z2, then construct ``fibered WZW models'' which allow us to explicitly couple current algebras for general groups and general levels to heterotic strings. This technology gives us a very general approach to handling heterotic compactifications with arbitrary principal bundles. It also gives us a physical realization of some elliptic genera constructed recently by Ando and Liu.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We examine to what extent heterotic string worldsheets can describe arbitrary E8xE8 gauge fields. | contribution 0.61 | 0.83 | 0.06 | unclear 0.58 |
| s1 | The traditional construction of heterotic strings builds each E8 via a Spin(16)/Z2 subgroup, typically realized as a current algebra by left-moving fermions, and as a result, only E8 gauge fields reducible to Spin(16)/Z2 gauge fields are directly realizable in standard constructions. | background 0.98 | 0.05 | 0.05 | asserted 1.00 |
| s2 | However, there exist perturbatively consistent E8 gauge fields which can not be reduced to Spin(16)/Z2, and so cannot be described within standard heterotic worldsheet constructions. | gap 0.63 | 0.18 | 0.06 | asserted 1.00 |
| s3 | A natural question to then ask is whether there exists any (0,2) SCFT that can describe such E8 gauge fields. | gap 0.94 | 0.06 | 0.04 | unclear 0.65 |
| s4 | To answer this question, we first show how each ten-dimensional E8 partition function can be built up using other subgroups than Spin(16)/Z2, then construct ``fibered WZW models'' which allow us to explicitly couple current algebras for general groups and general levels to heterotic strings. | method 0.76 | 0.95 | 0.25 | asserted 1.00 |
| s5 | This technology gives us a very general approach to handling heterotic compactifications with arbitrary principal bundles. | interpretation 0.63 | 0.87 | 0.42 | asserted 1.00 |
| s6 | It also gives us a physical realization of some elliptic genera constructed recently by Ando and Liu. | result 0.75 | 0.83 | 0.10 | asserted 0.91 |
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The paper
Original abstract
We examine to what extent heterotic string worldsheets can describe arbitrary E8xE8 gauge fields. The traditional construction of heterotic strings builds each E8 via a Spin(16)/Z2 subgroup, typically realized as a current algebra by left-moving fermions, and as a result, only E8 gauge fields reducible to Spin(16)/Z2 gauge fields are directly realizable in standard constructions. However, there exist perturbatively consistent E8 gauge fields which can not be reduced to Spin(16)/Z2, and so cannot be described within standard heterotic worldsheet constructions. A natural question to then ask is whether there exists any (0,2) SCFT that can describe such E8 gauge fields. To answer this question, we first show how each ten-dimensional E8 partition function can be built up using other subgroups than Spin(16)/Z2, then construct ``fibered WZW models'' which allow us to explicitly couple current algebras for general groups and general levels to heterotic strings. This technology gives us a very general approach to handling heterotic compactifications with arbitrary principal bundles. It also gives us a physical realization of some elliptic genera constructed recently by Ando and Liu.
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References
How the literature uses it
14 arXiv papers cite this in 21 sentences
Papers citing it · 15 sentences without a confident label
Builds on it 1 paper
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On the other hand, and in a dual sense, here we are looking at the higher brane version of Distler-Sharpe's heterotic string sigma models on $Q$ (instead of on $M$) [ref] , as an analogous “fibered” version of the heterotic NS5-brane sigma-model.
Topological actions via gauge variations of higher structures · Introduction · 0.98
Uses its data or values 1 paper
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From [ref] , [ref] , there are two integrable representations of $G_2$ at level 1, namely $[1]$, $[7]$, which obey [equation] We can write the ring as [equation] where we have identified $x$ with $[7]$.
Dilaton shifts, probability measures, and decomposition · $G/G$ model · 0.84
Cites it as background 4 papers
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A good reference for the relevant group theory is [ref] .] corresponding to removal of a node in $Ẽ_8$ affine Dynkin diagram.
Supersymmetric Hidden Sectors for Heterotic Standard Models · Induced Bundles · 0.99
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This can also be described via the notion of fibered WZW theory, string-theoretically realizing elliptic genera [ref] .
M-Theory with Framed Corners and Tertiary Index Invariants · Chromatic level 2: Heterotic corners and the $f$-invariant · 0.85
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While this covers many vacua, it is certainly not the most general situation, and there are certainly interesting compactifications based on $(n)$ bundles, as well as more general constructions, e.g. [ref] .
On marginal deformations of (0,2) non-linear sigma models · Concluding remarks · 0.89
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