摘要

In this paper, we develop an effective mutual Chern-Simons Landau-Ginzburg (MCSLG) theory to describe the continuous topological quantum phase transition (TQPT). In particular, we consider the TQPT between a spin-polarized phase (a state without topological order) and a Z(2) topologically ordered state. The TQPT is not induced by spontaneous symmetry breaking. Instead the Z(2) topological order is broken down by the condensation of Z(2) charged quasiparticles. By generalizing the hierarchy theory of fractional quantum Hall effect to Z(2) topological order, we show that the TQPT belongs to the universal class of three-dimensional Ising phase transition. In the end, we applied the MCSLG theory to the toric code model.