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arXiv 1402.0428quant-phphysics.optics
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宇称-时间对称性破缺:简并度的作用

Parity-Time Symmetry Breaking beyond One Dimension: The Role of Degeneracy

Li Ge, A. Douglas Stone

摘要:

本文研究了一维以上非厄米波动方程的简并性在宇称时间对称破缺中的作用。我们表明,如果频谱是退化的T-破缺的情况下,和T是打破了一个通用的方式(不保留其他离散对称性),那么标准的PT对称性破缺过渡不会发生,这意味着频谱是复杂的,即使对于无穷小的增益和损失的强度。然而,如果当T被破坏时施加额外的离散对称性X,如果X解耦所有简并模式,则整个谱的实性可以在有限区间上保持。当这只对简并谱的一个子集成立时,可以存在部分PT跃迁,其中该子集在T-破缺的有限区间上保持实数。如果光谱具有奇简并性,即使不施加额外的离散对称性,简并光谱的一部分也可以保持在对称相中,并且它们类似于原子物理学中的暗态。这些结果的例子说明了不同的T-破缺扰动的均匀介质盘和球,并给出了一个组理论分析在磁盘的情况下。最后,我们表明,多模耦合是能够恢复的T-对称相位在有限的T-打破。我们还分析了这些问题时,宇称算子被替换为另一个空间对称算子,发现的行为可以是定性的不同。

英文摘要:

We consider the role of degeneracy in Parity-Time (PT) symmetry breaking for non-hermitian wave equations beyond one dimension. We show that if the spectrum is degenerate in the absence of T-breaking, and T is broken in a generic manner (without preserving other discrete symmetries), then the standard PT-symmetry breaking transition does not occur, meaning that the spectrum is complex even for infinitesimal strength of gain and loss. However the realness of the entire spectrum can be preserved over a finite interval if additional discrete symmetries X are imposed when T is broken, if X decouple all degenerate modes. When this is true only for a subset of the degenerate spectrum, there can be a partial PT transition in which this subset remains real over a finite interval of T-breaking. If the spectrum has odd-degeneracy, a fraction of the degenerate spectrum can remain in the symmetric phase even without imposing additional discrete symmetries, and they are analogous to dark states in atomic physics. These results are illustrated by the example of different T-breaking perturbations of a uniform dielectric disk and sphere, and a group theoretical analysis is given in the disk case. Finally, we show that multimode coupling is capable of restoring the T-symmetric phase at finite T-breaking. We also analyze these questions when the parity operator is replaced by another spatial symmetry operator and find that the behavior can be qualitatively different.

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