NC Geometry and Fractional Branes

Details NC Geometry and Fractional Branes NC Geometry and Fractional Branes

2003-11-25

arxiv.org/abs/hep-th/0311245v1

Class.Quant.Grav. 20 (2003) 4447-4472

Physics

High Energy Physics

High Energy Physics - Theory

27 pages, 4figures

Scientific paper

Considering complex $n$-dimension Calabi-Yau homogeneous hyper-surfaces $% \mathcal{H}_{n}$ with discrete torsion and using Berenstein and Leigh algebraic geometry method, we study Fractional D-branes that result from stringy resolution of singularities. We first develop the method introduced in hep-th/0105229 and then build the non commutative (NC) geometries for orbifolds $\mathcal{O}=\mathcal{H}_{n}/\mathbf{Z}_{n+2}^{n}$ with a discrete torsion matrix $t_{ab}=exp[{\frac{i2\pi}{n+2}}{(\eta_{ab}-\eta_{ba})}]$, $\eta_{ab} \in SL(n,\mathbf{Z})$. We show that the NC manifolds $% \mathcal{O}^{(nc)}$ are given by the algebra of functions on the real $% (2n+4) $ Fuzzy torus $\mathcal{T}_{\beta_{ij}}^{2(n+2)}$ with deformation parameters $\beta_{ij}=exp{\frac{i2\pi}{n+2}}{[(\eta_{ab}^{-1}-\eta_{ba}^{-1})} q_{i}^{a} q_{j}^{b}]$ with $q_{i}^{a}$'s being charges of $% \mathbf{Z}_{n+2}^{n}$. We also give graphic rules to represent $\mathcal{O}% ^{(nc)}$ by quiver diagrams which become completely reducible at orbifold singularities. It is also shown that regular points in these NC geometries are represented by polygons with $(n+2)$ vertices linked by $(n+2)$ edges while singular ones are given by $(n+2)$ non connected loops. We study the various singular spaces of quintic orbifolds and analyze the varieties of fractional $D$ branes at singularities as well as the spectrum of massless fields. Explicit solutions for the NC quintic $\mathcal{Q}^{(nc)}$ are derived with details and general results for complex $n$ dimension orbifolds with discrete torsion are presented.

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