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    Competing PT potentials and re-entrant PT symmetric phase for a particle in a box

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    We investigate the effects of competition between two complex, PT\mathcal{PT}-symmetric potentials on the PT\mathcal{PT}-symmetric phase of a "particle in a box". These potentials, given by VZ(x)=iZsign(x)V_Z(x)=iZ\mathrm{sign}(x) and Vξ(x)=iξ[δ(x−a)−δ(x+a)]V_\xi(x)=i\xi[\delta(x-a)-\delta(x+a)], represent long-range and localized gain/loss regions respectively. We obtain the PT\mathcal{PT}-symmetric phase in the (Z,ξ)(Z,\xi) plane, and find that for locations ±a\pm a near the edge of the box, the PT\mathcal{PT}-symmetric phase is strengthened by additional losses to the loss region. We also predict that a broken PT\mathcal{PT}-symmetry will be restored by increasing the strength ξ\xi of the localized potential. By comparing the results for this problem and its lattice counterpart, we show that a robust PT\mathcal{PT}-symmetric phase in the continuum is consistent with the fragile phase on the lattice. Our results demonstrate that systems with multiple, PT\mathcal{PT}-symmetric potentials show unique, unexpected properties.Comment: 7 pages, 3 figure
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