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The proper Landau-Ginzburg potential is the open mirror map

Algebraic Geometry · Submitted 26 Apr 2022

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

The authors' main claim We show that this proper superpotential equals the open mirror map for outer Aganagic-Vafa branes in the canonical bundle $K_X$, in framing zero.

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arXiv ID2204.12249 (version 3)
Pith IDLVRQZ5VA, Pith's permanent record of this paper and its review
CitationEric Zaslow, Helge Ruddat, Tim Gr\"afnitz. "The proper Landau-Ginzburg potential is the open mirror map." arXiv:2204.12249 (2022). https://pith.science/paper/LVRQZ5VA
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arXiv listing abstract v3. Results and the main claim are underlined; .

The mirror dual of a smooth toric Fano surface $X$ equipped with an anticanonical divisor $E$ is a Landau-Ginzburg model with superpotential, W. Carl-Pumperla-Siebert give a definition of the the superpotential in terms of tropical disks using a toric degeneration of the pair $(X,E)$. When $E$ is smooth, the superpotential is proper. We show that this proper superpotential equals the open mirror map for outer Aganagic-Vafa branes in the canonical bundle $K_X$, in framing zero. As a consequence, the proper Landau-Ginzburg potential is a solution to the Lerche-Mayr Picard-Fuchs equation. Along the way, we prove a generalization of a result about relative Gromov-Witten invariants by Cadman-Chen to arbitrary genus using the multiplication rule of quantum theta functions. In addition, we generalize a theorem of Hu that relates Gromov-Witten invariants of a surface under a blow-up from the absolute to the relative case. One of the two proofs that we give introduces birational modifications of a scattering diagram. We also demonstrate how the Hori-Vafa superpotential is related to the proper superpotential by mutations from a toric chamber to the unbounded chamber of the scattering diagram.

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What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The mirror dual of a smooth toric Fano surface $X$ equipped with an anticanonical divisor $E$ is a Landau-Ginzburg model with superpotential, W. background 1.00 0.09 0.05 asserted 1.00
s1 Carl-Pumperla-Siebert give a definition of the the superpotential in terms of tropical disks using a toric degeneration of the pair $(X,E)$. background 1.00 0.05 0.02 asserted 1.00
s2 When $E$ is smooth, the superpotential is proper. background 0.65 0.16 0.05 asserted 1.00
s3 We show that this proper superpotential equals the open mirror map for outer Aganagic-Vafa branes in the canonical bundle $K_X$, in framing zero. result 0.95 0.95 0.82 asserted 1.00
s4 As a consequence, the proper Landau-Ginzburg potential is a solution to the Lerche-Mayr Picard-Fuchs equation. result 0.83 0.83 0.21 asserted 1.00
s5 Along the way, we prove a generalization of a result about relative Gromov-Witten invariants by Cadman-Chen to arbitrary genus using the multiplication rule of quantum theta functions. contribution 0.77 0.95 0.04 asserted 1.00
s6 In addition, we generalize a theorem of Hu that relates Gromov-Witten invariants of a surface under a blow-up from the absolute to the relative case. contribution 0.85 0.93 0.03 asserted 1.00
s7 One of the two proofs that we give introduces birational modifications of a scattering diagram. method 0.85 0.93 0.03 asserted 0.99
s8 We also demonstrate how the Hori-Vafa superpotential is related to the proper superpotential by mutations from a toric chamber to the unbounded chamber of the scattering diagram. result 0.66 0.89 0.05 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

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The paper
Original abstract

The mirror dual of a smooth toric Fano surface $X$ equipped with an anticanonical divisor $E$ is a Landau-Ginzburg model with superpotential, W. Carl-Pumperla-Siebert give a definition of the the superpotential in terms of tropical disks using a toric degeneration of the pair $(X,E)$. When $E$ is smooth, the superpotential is proper. We show that this proper superpotential equals the open mirror map for outer Aganagic-Vafa branes in the canonical bundle $K_X$, in framing zero. As a consequence, the proper Landau-Ginzburg potential is a solution to the Lerche-Mayr Picard-Fuchs equation. Along the way, we prove a generalization of a result about relative Gromov-Witten invariants by Cadman-Chen to arbitrary genus using the multiplication rule of quantum theta functions. In addition, we generalize a theorem of Hu that relates Gromov-Witten invariants of a surface under a blow-up from the absolute to the relative case. One of the two proofs that we give introduces birational modifications of a scattering diagram. We also demonstrate how the Hori-Vafa superpotential is related to the proper superpotential by mutations from a toric chamber to the unbounded chamber of the scattering diagram.

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6 arXiv papers cite this in 20 sentences

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

Papers citing it · 16 sentences without a confident label

Builds on it 1 paper
Uses its data or values 1 paper
  • gives the broken lines to compute the log Gromov-Witten invariant $R_1,5(ℙ^2,E)=25$ of conics meeting $E$ in a fixed point with multiplicity $1$ and another point with multiplicity $5$ as in [ref] , Appendix B.

    Counting (tropical) curves via scattering.sage · Broken lines · 0.82

Cites it as background 2 papers

What it cites · 71 sentences without a confident label

Builds on 1 paper
  • In this section, we generalize the theta function multiplication rule from its genus zero version in [ref] , assuming $B=2$, to arbitrary genus and then use the rule to prove relations among the two-point invariants that we introduced in the previous section.

    Theta functions on varieties with effective anti-canonical class · Theta calculations · 1.00

Uses the method or tool of 3 papers
  • Since this potential can be easily computed in the central chamber to agree with the Hori–Vafa superpotential, we can fix an order $k$ for the wall structure and relate that to the function $M(Q)$ mod $t^k$ by a finite series of mutations à la [ref] .

    A tropical view on Landau-Ginzburg models · Steps of the proof and auxiliary results · 1.00

  • For a trivalent vertex $V∈V(Γ)$ define, with $u_(V,E)∈ι_⋆Λ_h(V)$ as in [ref] , Definition 3.3, [equation] where $E_1,E_2$ are any two edges adjacent to $V$.

    Tropical correspondence for smooth del Pezzo log Calabi-Yau pairs · Tropical curves · 0.84

  • If two rays intersect with determinant $m$, the scattering diagram is locally isomorphic via a change of lattice (see [ref] , Proposition C.13) to the one obtained from the “standard” scattering diagram with function $1+atx^m$ and $1+bty^m$, for some $a,b∈ℤ$.

    Canonical bases for cluster algebras · Steps of the proof and auxiliary results · 0.80

Compares with 3 papers
  • The second difference is that in [ref] the general fiber has trivial log structure, while our general fiber $X$ carries the divisorial log structure from the divisor $E⊂X$.

    The degeneration formula for stable log maps · Relating one point invariants to multi point invariants · 0.97

  • The computations of [ref] agree with Mayr's calculations using differential equations [ref] , a method further developed in [ref] .

    On N=1 Mirror Symmetry for Open Type II Strings · Steps of the proof and auxiliary results · 0.93

  • As mentioned in Remark [ref], similar results were obtained for moment fibers, rather than Aganagic–Vafa outer branes, in [ref] — see their Remark 5.7.

    SYZ mirror symmetry for toric Calabi-Yau manifolds · The case of $^2$: Picard–Fuchs equations and mirror maps · 0.87

Cites as background 14 papers
  • Aganagic–Vafa studied a class of Lagrangian A-branes in a toric $K_X$ and their mirror B-branes: the open mirror map relates parameters for their common moduli space [ref] .

    Mirror Symmetry, D-Branes and Counting Holomorphic Discs · Introduction and Summary · 0.96

  • By “open mirror map,” we mean the relation between complex and symplectic open parameters defined by the logarithmic solution to the Picard–Fuchs differential equations of Lerche–Mayr [ref] — see Section [ref].

    On N=1 Mirror Symmetry for Open Type II Strings · Introduction and Summary · 0.80

  • The function $M(Q)$ originally appeared in the work of Aganagic–Klemm–Vafa [ref] as the open mirror map relating Aganagic–Vafa branes [ref] on the canonical bundle $K_^2$ and its mirror, and was used to determine open Gromov–Witten invariants in [ref] .

    Disk Instantons, Mirror Symmetry and the Duality Web · Introduction and Summary · 0.89

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