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Cubics, Integrable Systems, and Calabi-Yau Threefolds
alg-geom · Submitted 9 Aug 1994
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In this work we construct an analytically completely integrable Hamiltonian system which is canonically associated to any family of Calabi-Yau threefolds.
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The abstract, sentence by sentence
In this work we construct an analytically completely integrable Hamiltonian system which is canonically associated to any family of Calabi-Yau threefolds. The base of this system is a moduli space of gauged Calabi-Yaus in the family, and the fibers are Deligne cohomology groups (or intermediate Jacobians) of the threefolds. This system has several interesting properties: the multivalued sections obtained as Abel-Jacobi images, or ``normal functions'', of a family of curves on the generic variety of the family, are always Lagrangian; the natural affine coordinates on the base, which are used in the mirror correspondence, arise as action variables for the integrable system; and the Yukawa cubic, expressing the infinitesimal variation of Hodge structure in the family, is essentially equivalent to the symplectic structure on the total space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In this work we construct an analytically completely integrable Hamiltonian system which is canonically associated to any family of Calabi-Yau threefolds. | contribution 0.99 | 0.95 | 0.78 | asserted 1.00 |
| s1 | The base of this system is a moduli space of gauged Calabi-Yaus in the family, and the fibers are Deligne cohomology groups (or intermediate Jacobians) of the threefolds. | contribution 0.82 | 0.78 | 0.09 | asserted 1.00 |
| s2 | This system has several interesting properties: the multivalued sections obtained as Abel-Jacobi images, or ``normal functions'', of a family of curves on the generic variety of the family, are always Lagrangian; the natural affine coordinates on the base, which are used in the mirror correspondence, arise as action variables for the integrable system; and the Yukawa cubic, expressing the infinitesimal variation of Hodge structure in the family, is essentially equivalent to the symplectic structure on the total space. | result 0.94 | 0.81 | 0.19 | asserted 1.00 |
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The paper
Original abstract
In this work we construct an analytically completely integrable Hamiltonian system which is canonically associated to any family of Calabi-Yau threefolds. The base of this system is a moduli space of gauged Calabi-Yaus in the family, and the fibers are Deligne cohomology groups (or intermediate Jacobians) of the threefolds. This system has several interesting properties: the multivalued sections obtained as Abel-Jacobi images, or ``normal functions'', of a family of curves on the generic variety of the family, are always Lagrangian; the natural affine coordinates on the base, which are used in the mirror correspondence, arise as action variables for the integrable system; and the Yukawa cubic, expressing the infinitesimal variation of Hodge structure in the family, is essentially equivalent to the symplectic structure on the total space.
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References
How the literature uses it
9 arXiv papers cite this in 18 sentences
Papers citing it · 8 sentences without a confident label
Uses its method or tool 1 paper
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We outline a proof following [ref] ; for the original proof see [ref] .
Aspects of Calabi-Yau Integrable and Hitchin Systems · Compact Calabi–Yau integrable systems · 0.80
Compares with it 1 paper
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With these methods we construct Calabi–Yau integrable systems from complete families of compact Calabi–Yau threefolds in a different way than originally done by Donagi–Markman [ref] .
Aspects of Calabi-Yau Integrable and Hitchin Systems · Structure of the notes · 0.98
Cites it as background 6 papers
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The low-energy theory around a generic point on a rank-$r$ CB is captured by a fibration of rank-$r$ abelian varieties [ref] .
Completely (iso-)split scale-invariant Coulomb branch geometries are isotrivial · Introduction · 0.88
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The SK structure of $$ is captured by a holomorphic algebraically completely integrable Hamiltonian system [ref] whose complex phase space we call the total space, $X$, of the CB.
Flavor symmetries and the topology of special K\"ahler structures at rank 1 · Generalization to higher ranks · 0.89
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Instead, the natural invariant object is the holomorphic 2-form [ref] [equation] defined on the total space of the elliptic fibration.
Seiberg-Witten geometries for Coulomb branch chiral rings which are not freely generated · Seiberg Witten curve and form · 0.80
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