Individual eigenvalue distributions of chiral random two-matrix theory and the determination of Fπ

被引:12
|
作者
Akemann, G. [1 ,2 ]
Damgaard, P. H. [3 ]
机构
[1] Brunel Univ, Dept Math Sci, Uxbridge UB8 3PH, Middx, England
[2] Brunel Univ, BURSt Res Ctr, Uxbridge UB8 3PH, Middx, England
[3] Niels Bohr Int Acad, Niels Bohr Inst, DK-2100 Copenhagen, Denmark
来源
JOURNAL OF HIGH ENERGY PHYSICS | 2008年 / 03期
关键词
matrix models; lattice QCD; chiral lagrangians;
D O I
10.1088/1126-6708/2008/03/073
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
Dirac operator eigenvalues split into two when subjected to two different external vector sources. In a specific finite-volume scaling regime of gauge theories with fermions, this problem can be mapped to a chiral Random Two-Matrix Theory. We derive analytical expressions to leading order in the associated finite-volume expansion, showing how individual Dirac eigenvalue distributions and their correlations equivalently can be computed directly from the effective chiral Lagrangian in the epsilon-regime. Because of its equivalence to chiral Random Two-Matrix Theory, we use the latter for all explicit computations. On the mathematical side, we define and determine gap probabilities and individual eigenvalue distributions in that theory at finite N, and also derive the relevant scaling limit as N is taken to infinity. In particular, the gap probability for one Dirac eigenvalue is given in terms of a new kernel that depends on the external vector source. This expression may give a new and simple way of determining the pion decay constant F-pi from lattice gauge theory simulations.
引用
收藏
页数:28
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