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Superpotentials for Vector Bundle Moduli
High Energy Physics - Theory · Submitted 19 May 2002
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We present a method for explicitly computing the non-perturbative superpotentials associated with the vector bundle moduli in heterotic superstrings and M-theory.
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The abstract, sentence by sentence
We present a method for explicitly computing the non-perturbative superpotentials associated with the vector bundle moduli in heterotic superstrings and M-theory. This method is applicable to any stable, holomorphic vector bundle over an elliptically fibered Calabi-Yau threefold. For specificity, the vector bundle moduli superpotential, for a vector bundle with structure group G=SU(3), generated by a heterotic superstring wrapped once over an isolated curve in a Calabi-Yau threefold with base B=F1, is explicitly calculated. Its locus of critical points is discussed. Superpotentials of vector bundle moduli potentially have important implications for small instanton phase transitions and the vacuum stability and cosmology of superstrings and M-theory.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a method for explicitly computing the non-perturbative superpotentials associated with the vector bundle moduli in heterotic superstrings and M-theory. | contribution 0.97 | 0.95 | 0.51 | asserted 1.00 |
| s1 | This method is applicable to any stable, holomorphic vector bundle over an elliptically fibered Calabi-Yau threefold. | method 0.45 | 0.63 | 0.10 | asserted 1.00 |
| s2 | For specificity, the vector bundle moduli superpotential, for a vector bundle with structure group G=SU(3), generated by a heterotic superstring wrapped once over an isolated curve in a Calabi-Yau threefold with base B=F1, is explicitly calculated. | result 0.68 | 0.95 | 0.24 | asserted 1.00 |
| s3 | Its locus of critical points is discussed. | result 0.68 | 0.84 | 0.06 | asserted 0.74 |
| s4 | Superpotentials of vector bundle moduli potentially have important implications for small instanton phase transitions and the vacuum stability and cosmology of superstrings and M-theory. | interpretation 1.00 | 0.11 | 0.17 | hedged possibility 0.99 |
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The paper
Original abstract
We present a method for explicitly computing the non-perturbative superpotentials associated with the vector bundle moduli in heterotic superstrings and M-theory. This method is applicable to any stable, holomorphic vector bundle over an elliptically fibered Calabi-Yau threefold. For specificity, the vector bundle moduli superpotential, for a vector bundle with structure group G=SU(3), generated by a heterotic superstring wrapped once over an isolated curve in a Calabi-Yau threefold with base B=F1, is explicitly calculated. Its locus of critical points is discussed. Superpotentials of vector bundle moduli potentially have important implications for small instanton phase transitions and the vacuum stability and cosmology of superstrings and M-theory.
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References
How the literature uses it
20 arXiv papers cite this in 32 sentences
Papers citing it · 25 sentences without a confident label
Uses its method or tool 1 paper
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The bundle $V|_σ$ can be obtained from the spectral data $(C, N|_C)$ as follows [ref]
Dynamically SUSY Breaking SQCD on F-Theory Seven-Branes · The Matter Localized on the Curve · 0.92
Cites it as background 5 papers
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This has been pursued in works such as [ref] .
Elusive Worldsheet Instantons in Heterotic String Compactifications · Introduction · 0.84
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Expression of this type of familiar from `physical gauge' calculations of corrections to the spacetime superpotential in heterotic compactifications due to worldsheet instantons [ref] .
Heterotic twistor-string theory · Witten's twistor-string: D5-D5, D5-D1 and D1-D1 strings · 0.84
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For this reason they have been studied in string theory from the early days on (see for instance [ref] ), where particular attention was given to instanton corrections to the superpotential of the four-dimensional $N=1$ supersymmetric effective action, as these corrections influence the vacuum structure of the string compactification.
Power Towers of String Instantons for N=1 Vacua · Introduction · 0.99
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