Abstract

We consider a topological superconducting wire and use the string order parameter to investigate the spatiotemporal evolution of the topological order upon a quantum quench across the critical point. We also analyze the propagation of the initially localized Majorana bound states after the quench, in order to examine the connection between the topological order and the unpaired Majorana states, which has been well established at equilibrium but remains illusive in dynamical situations. It is found that after the quench the string order parameters decay over a finite time and that the decaying behavior is universal, independent of the wire length and the final value of the chemical potential (the quenching parameter). It is also found that the topological order is revived repeatedly although the amplitude gradually decreases. Further, the topological order can propagate into the region which was initially in the nontopological state. It is observed that all these behaviors are in parallel and consistent with the propagation and dispersion of the Majorana wave functions. Finally, we propose local probing methods which can measure the nonlocal topological order.

Highlights

  • Landau’s symmetry-breaking theory [1, 2, 3] has long provided a universal paradigm for the states of matter and their transitions

  • This early decaying behavior is universal in the sense that it does not depend on the wire length and the final value of the chemical potential

  • We summarize the two characteristic behaviors of the string order parameter uncovered in Fig. 3: (i) The topological orders defined by Eqs. (5), (6), and (7) do not die away immediately after the quench, but instead decay with time before they vanish completely

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Summary

Introduction

Landau’s symmetry-breaking theory [1, 2, 3] has long provided a universal paradigm for the states of matter and their transitions. It has been shown that the original Kibble-Zurek scaling form does not hold for the topological phase transitions [25, 26] but one can generalize it by properly taking into account the multi-level structure due to the Majorana bound states [27] None of these approaches directly measures the dynamic topological order; they either resort to the fidelity to the ground state or to the number of topological defects. It discusses the dynamical aspects of the topological order in terms of the propagation of the Majorana wave functions.

Topological Superconducting Wires and Topological Order
Topological Order
Time Evolution and Majorana Correlation Matrix
General Structure of Majorana Correlation Matrix
Quench Dynamics
Time Evolution of Topological Order in Uniform Wire
Propagation of Topological Order into Non-Topological Regions
Experimental Detection of Topological Order
Conclusion

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