A study of quantum Berezinskii-Kosterlitz-Thouless transition for parity-time symmetric quantum criticality

The Berezinskii-Kosterlitz-Thouless (BKT) mechanism governs the critical behavior of a wide range of many-body systems. We show here that this phenomenon is not restricted to conventional many body system but also for the strongly correlated parity-time (PT) symmetry quantum criticality. We show explicitly behaviour of topological excitation for the real and imaginary part of the potential are different through the analysis of second order and third order renormalization group (RG). One of the most interesting feature that we observe from our study the presence of hidden QBKT and also conventional QBKT for the real part of the potential whereas there is no such evidence for the imaginary part of the potential. We also present the exact solution for the RG flow lines. We show explicitly how the physics of single field double frequencies sine-Gordon Hamiltonian effectively transform to the dual field double frequencies sine-Gordon Hamiltonian for a certain regime of parameter space. This is the first example in any quantum many body systems. We present the results of second order and third order RG flow results explicitly for the real and imaginary part of the potential. This PT symmetric system can be experimentally tested in ultra-cold atoms. This work provides a new perspective for the PT symmetric quantum criticality.

Automated summary

The BKT mechanism applies not only to conventional many-body systems, but also to strongly correlated PT symmetry quantum criticality. We observe the presence of hidden QBKT and conventional QBKT for the real part of the potential, with no evidence for the imaginary part. Additionally, we provide exact solutions for the RG flow lines.