Abstract

We study the phase-diagram of a parity and time-reversal (PT) symmetric tight-binding chain with NN sites and hopping energy JJ, in the presence of two impurities with imaginary potentials ±iγ\pm iγ located at arbitrary (P-symmetric) positions (m,mˉ=N+1−m)(m, \bar{m}=N+1-m) on the chain where m≤N/2m\leq N/2. We find that except in the two special cases where impurities are either the farthest or the closest, the PT-symmetric region - defined as the region in which all energy eigenvalues are real - is algebraically fragile. We analytically and numerically obtain the critical impurity potential γPTγ_{PT} and show that γPT∝1/N→0γ_{PT}\propto 1/N\rightarrow 0 as N→∞N\rightarrow\infty except in the two special cases. When the PT symmetry is spontaneously broken, we find that the maximum number of complex eigenvalues is given by 2m2m. When the two impurities are the closest, we show that the critical impurity strength γPTγ_{PT} in the limit N→∞N\rightarrow\infty approaches JJ (J/2J/2) provided that NN is even (odd). For an even NN the PT symmetry is maximally broken whereas for an odd NN, it is sequentially broken. Our results show that the phase-diagram of a PT-symmetric tight-binding chain is extremely rich and that, in the continuum limit, this model may give rise to new PT-symmetric Hamiltonians.

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