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Quasimap SYZ for toric Calabi-Yau manifolds

Symplectic Geometry · Submitted 6 Apr 2017

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We show that the resulting SYZ mirror coincides with the one written down via physical means (as expected).

how it is stated · asserted 1.00 read the record →

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arXiv ID1704.01730 (version 2)
Pith IDWZAYQENZ, Pith's permanent record of this paper and its review
CitationKwokwai Chan. "Quasimap SYZ for toric Calabi-Yau manifolds." arXiv:1704.01730 (2017). https://pith.science/paper/WZAYQENZ
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 2,318 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.10 · human participants 0.01 · controlled comparison 0.16 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.92 · mentions code or data availability 0.02.

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arXiv listing abstract v2. Results and the main claim are underlined; .

In this note, we study the SYZ mirror construction for a toric Calabi-Yau manifold using instanton corrections coming from Woodward's quasimap Floer theory instead of Fukaya-Oh-Ohta-Ono's Lagrangian Floer theory. We show that the resulting SYZ mirror coincides with the one written down via physical means (as expected).

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 In this note, we study the SYZ mirror construction for a toric Calabi-Yau manifold using instanton corrections coming from Woodward's quasimap Floer theory instead of Fukaya-Oh-Ohta-Ono's Lagrangian Floer theory. contribution 0.91 0.76 0.12 asserted 0.86
s1 We show that the resulting SYZ mirror coincides with the one written down via physical means (as expected). result 0.99 0.90 0.81 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from proof or derivation 0.97.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

In this note, we study the SYZ mirror construction for a toric Calabi-Yau manifold using instanton corrections coming from Woodward's quasimap Floer theory instead of Fukaya-Oh-Ohta-Ono's Lagrangian Floer theory. We show that the resulting SYZ mirror coincides with the one written down via physical means (as expected).

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What this paper does with the arXiv papers it cites

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

What it cites · 4 sentences without a confident label

Compares with 2 papers
  • The function $W^QF$ coincides with the Givental-Hori-Vafa superpotential [ref] for the toric manifold $X$.

    Mirror Symmetry · Woodward's quasimap Floer theory · 0.97

  • Notice that the quasimap SYZ mirror family [ref] is entirely written in terms of symplectic-geometric information such as complexified Kähler parameters and quasidisk invariants of $X$, and it coincides with the mirror [ref] predicted by physical arguments [ref] .

    D-Branes And Mirror Symmetry · Wall-crossing for quasidisk invariants and the SYZ mirror · 0.97

Cites as background 4 papers
  • In [ref] (see also [ref] ), Woodward developed a quasimap Floer theory as the zero-area limit of Frauenfelder's gauged Lagrangian Floer theory [ref] .

    Gauged Floer theory of toric moment fibers · Woodward's quasimap Floer theory · 0.87

  • The mirror of a toric Calabi-Yau manifold $X$ is predicted to be a family of affine hypersurfaces in $^2 ×(^×)^n-1$ [ref] explicitly written as [equation] where the coefficients $Č_i ∈$ are constants (without loss of generality, we will set $Č_m = 1$) subject to the constraints [equation] here $t = (t_1, …, t_r)$ are coordinates on the mirror complex moduli $ℳ̌_B := 𝕂^∨⊗_ ^×≅(^×)^r$. $X̌_t$ is Calabi-Yau since [equation] is a nowhere vanishing holomorphic volume form on $X̌_t$.

    Mirror Symmetry · Toric Calabi-Yau manifolds and their physical mirrors · 0.89

  • The mirror of a toric Calabi-Yau manifold $X$ is predicted to be a family of affine hypersurfaces in $^2 ×(^×)^n-1$ [ref] explicitly written as [equation] where the coefficients $Č_i ∈$ are constants (without loss of generality, we will set $Č_m = 1$) subject to the constraints [equation] here $t = (t_1, …, t_r)$ are coordinates on the mirror complex moduli $ℳ̌_B := 𝕂^∨⊗_ ^×≅(^×)^r$. $X̌_t$ is Calabi-Yau since [equation] is a nowhere vanishing holomorphic volume form on $X̌_t$.

    D-Branes And Mirror Symmetry · Toric Calabi-Yau manifolds and their physical mirrors · 0.89

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