Dyson's Instability in Lattice Gauge Theory

We discuss Dyson’s argument that the vacuum is unstable under a change g^2 ->

g^2, in the context of lattice gauge theory. For compact gauge groups, the partition function is well defined at negative g^2, but the average plaquette P has a discontinuity when g^2 changes sign. This reflects a change of vacuum rather than a loss of vacuum. In addition, P has poles in the complex g^2 plane, located at the complex zeros of the partition function (Fisher’s zeros). We discuss the relevance of these singularities for lattice perturbation theory. We present new methods to locate Fisher’s zeros using numerical values for the density of state in SU(2) and U(1) pure gauge theory. We briefly discuss similar issues for O(N) nonlinear sigma models where the local integrals are also over compact spaces.

We discuss Dyson’s argument that the vacuum is unstable under a change g^2 ->

g^2, in the context of lattice gauge theory. For compact gauge groups, the partition function is well defined at negative g^2, but the average plaquette P has a discontinuity when g^2 changes sign. This reflects a change of vacuum rather than a loss of vacuum. In addition, P has poles in the complex g^2 plane, located at the complex zeros of the partition function (Fisher’s zeros). We discuss the relevance of these singularities for lattice perturbation theory. We present new methods to locate Fisher’s zeros using numerical values for the density of state in SU(2) and U(1) pure gauge theory. We briefly discuss similar issues for O(N) nonlinear sigma models where the local integrals are also over compact spaces.

文献摘要