Quantum Periods and Toric Landau-Ginzburg Models in Threefold Divisorial Contractions

arXiv Math · · 1 min read · Natural Sciences

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Key Takeaways

  • A regularized period identity is proven for divisorial contractions of terminal Fano threefolds.
  • The identity holds under specific conditions for the center of contraction (smooth point, terminal quotient point, cA/n point, or a smooth curve with cA/cA/n singularities).
  • The identity provides a mirror approach for computing Sarkisov links and higher syzygies of central models of dimension 3.

Why This Matters

This research provides a mirror approach for computing Sarkisov links and higher syzygies in three-dimensional central models. This method contributes to the theoretical framework for analyzing complex geometric transformations.

Overview

This study investigates quantum periods and toric Landau-Ginzburg (LG) models in the context of divisorial contractions involving terminal Fano threefolds. The core of the research establishes a regularized period identity under specific conditions for the center of contraction.

Research Context

The research focuses on transformations between $\mathbb{Q}$-factorial Fano threefolds, denoted as $g:Y \rightarrow X$, where $g$ represents a divisorial contraction. Both $Y$ and $X$ are characterized by ordinary terminal singularities. A key element of this contraction is the exceptional divisor, $E$. The investigation is conditioned on the nature of the center of contraction, which is assumed to be one of the following:

  • A smooth point.
  • A terminal quotient point.
  • A point of type cA/n.
  • A smooth curve with singularities of type cA or cA/n.

Approach

The approach involves analyzing and proving a specific regularized period identity. This identity relates the regularized quantum periods of two different geometric configurations. Specifically, the study aims to demonstrate that:

$$ \lim_{r\to+\infty}\hat{G}_{Y,rE}(t)=\hat{G}_X(t) $$

Here, $\hat{G}_{Y,rE}(t)$ represents the regularized quantum period associated with the pair $(Y,rE)$, and $\hat{G}_X(t)$ denotes the regularized quantum period of $X$. The limit as $r$ approaches positive infinity is central to this identity.

Findings

The primary finding is the proof of the regularized period identity:

$$ \lim_{r\to+\infty}\hat{G}_{Y,rE}(t)=\hat{G}_X(t) $$

This identity holds when the center of the divisorial contraction $g:Y \rightarrow X$ meets the specified conditions: being a smooth point, a terminal quotient point, a point of type cA/n, or a smooth curve with singularities of type cA or cA/n.

Why This Matters

The established regularized period identity provides a mirror approach. This approach is instrumental for the computation of Sarkisov links and higher syzygies, specifically within central models of dimension 3.

Research Information

Institution
arXiv Math
Original Study
View Publication
Source
arXiv Math

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