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arXiv 2610.13331math.AG
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Gamma猜想II与二次射影丛的显式Stokes数据

Gamma conjecture II and explicit Stokes data for a quadric projective bundle

School of Mathematics, Southwest Jiaotong University(西南交通大学数学学院)

Xiaobin Li

AI总结:

该研究针对Fano四维簇$X=\PP_{Q^3}(\OO\oplus\OO(1))$的量子微分方程,通过Mellin-Bessel积分等方法证明Gamma猜想II,确定其Stokes等数据,并推广到更高维的二次射影丛情形。

摘要:

我们研究Fano四维簇$X=\PP_{Q^3}(\OO\oplus\OO(1))$的量子微分方程的连接问题,该问题旨在将其典范渐近解与例外对象对应并计算相关的Stokes数据。我们采用精确的Mellin-Bessel积分表示、宽度大于$\pi$的扇区上的一致向量渐近,以及保持Gamma框架的解析延拓。上同调手征对称性与例外集合的突变使全部八个截面处于同一相位。这证明了$X$的Gamma猜想II,并确定了单位Novikov点与指定容许相位下的满例外集合及其Stokes矩阵、中心连接矩阵。手征对称性还给出了平坦对称双线性配对、Stokes矩阵的正交性恒等式,以及满旋转下单值群矩阵的整幂幺平方根。我们得到了相反相位下连接数据的显式公式;在Gamma格上,半旋转通过与反典范丛的平方根张量积作用。相同的旋量积分变换为$\PP_{Q^{2m+1}}(\OO\oplus\OO(1))$($m\geq1$)在具有不同谱的正参数下构造了两个典范Gamma截面,其扇区开度大于$\pi$,且首项常数与维度无关。

英文摘要:

We study the connection problem for the quantum differential equation of the Fano fourfold $X=\PP_{Q^3}(\OO\oplus\OO(1))$. The problem is to identify its canonical asymptotic solutions with exceptional objects and compute the associated Stokes data. We use exact Mellin--Bessel integral representations and uniform vector asymptotics on sectors wider than $π$, followed by analytic continuation that preserves the Gamma framing. Cohomological chiral symmetry and mutations of exceptional collections put all eight sections at a common phase. This proves Gamma conjecture II for $X$ and determines a full exceptional collection and its Stokes and central connection matrices at the unit Novikov point and a specified admissible phase. The chiral symmetry also gives a flat symmetric bilinear pairing, an orthogonality identity for the Stokes matrix, and an integral unipotent square root of the monodromy matrix for a full turn. We obtain explicit formulas for the connection data at the opposite phase; on the Gamma lattice, the half-turn acts by tensoring with a square root of the anticanonical bundle. The same spinor integral transform constructs two canonical Gamma sections for $\PP_{Q^{2m+1}}(\OO\oplus\OO(1))$, $m\geq1$, at positive parameters with distinct spectrum. Their sectors have opening greater than $π$, and their leading constants are independent of the dimension.

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