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arXiv 1906.09362math-phhep-thmath.MPmath.QA
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随机有限非交换几何与拓扑递归

Random Finite Noncommutative Geometries and Topological Recursion

Shahab Azarfar, Masoud Khalkhali

AI总结:

本文用斑块化拓扑递归研究类型 (1,0) 随机矩阵几何,推导多迹 1-Hermitian 矩阵模型的 Schwinger-Dyson 方程,并给出谱曲线基本双微分的显式表达。

摘要:

本文利用 blobbed topological recursion(斑块化拓扑递归)理论,研究有限非交换空间上的量子引力模型。该模型基于一类特定的随机有限实谱三元组 ${(\mathcal{A}, \mathcal{H}, D, \gamma, J)}$,称为类型 ${(1,0)}$ 的随机矩阵几何;其中费米子空间 ${(\mathcal{A}, \mathcal{H}, \gamma, J)}$ 固定,并在 Dirac 算子的模空间上赋予形如 ${e^{-\mathcal{S}(D)}\mathrm{d}D}$ 的分布。作用量泛函 ${\mathcal{S}(D)}$ 被视为若干项之和,每项具有 ${\prod_{i=1}^s \mathrm{Tr}(D^{n_i})}$ 的形式,其中任意 ${s\geqslant 1}$。我们通过微分几何方法,推导了相应多迹形式 1-Hermitian 矩阵模型的连通关联函数 ${W_n}$ 所满足的 Schwinger-Dyson 方程。结果表明,${W_n}$ 的大 $N$ 展开系数 ${W_{g,n}}$ 枚举了称为 stuffed maps(填充映射)的离散曲面,其构造块具有特定拓扑。本文还详细研究了模型的谱曲线 ${(\Sigma,\omega_{0,1},\omega_{0,2})}$;特别地,我们依据模型的形式参数推导了基本对称双微分 ${\omega_{0,2}}$ 的显式表达式。

英文摘要:

In this paper we investigate a model for quantum gravity on finite noncommutative spaces using the theory of blobbed topological recursion. The model is based on a particular class of random finite real spectral triples ${(\mathcal{A}, \mathcal{H}, D , γ, J) \,}$, called random matrix geometries of type ${(1,0) \,}$, with a fixed fermion space ${(\mathcal{A}, \mathcal{H}, γ, J) \,}$, and a distribution of the form ${e^{- \mathcal{S} (D)} {\mathop{}\!\mathrm{d}} D}$ over the moduli space of Dirac operators. The action functional ${\mathcal{S} (D)}$ is considered to be a sum of terms of the form ${\prod_{i=1}^s \mathrm{Tr} \left( {D^{n_i}} \right)}$ for arbitrary ${s \geqslant 1 \,}$. The Schwinger-Dyson equations satisfied by the connected correlators ${W_n}$ of the corresponding multi-trace formal 1-Hermitian matrix model are derived by a differential geometric approach. It is shown that the coefficients ${W_{g,n}}$ of the large $N$ expansion of ${W_n}$'s enumerate discrete surfaces, called stuffed maps, whose building blocks are of particular topologies. The spectral curve ${\left( {Σ, ω_{0,1} , ω_{0,2}} \right)}$ of the model is investigated in detail. In particular, we derive an explicit expression for the fundamental symmetric bidifferential ${ω_{0,2}}$ in terms of the formal parameters of the model.

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