2015
DOI: 10.1103/physreva.91.033815
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Interplay of disorder andPTsymmetry in one-dimensional optical lattices

Abstract: We study a one-dimensional binary optical lattice in the presence of diagonal disorder and alternating gain and loss, and examine the light transport phenomena for localized and extended input beams. In the pure PT -symmetric case, we derive an exact expression for the behavior of light localization in terms of typical parameters of the system. Within the PT -symmetric region light localization becomes constant as a function of the strength of the gain and loss parameter, but outside the PT -symmetric window, … Show more

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Cited by 41 publications
(25 citation statements)
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“…The nonlinear effects in PT-symmetric systems can be utilized for an efficient control of light including all-optical low-threshold switching and unidirectional invisibility [24,56,57]. The possibility to engineer PT-symmetric oligomers, which may include nonlinearity, triggers a broad variety of studies on both the few-site systems and entire PT-symmetric lattices, including onedimensional PT-symmetric dimer [35,58], trimer [58,59], quadrimer [58,60], 2D PT-symmetric plaquettes [60,61], PT-symmetric finite/infinite chains [62][63][64][65], necklaces [66] and multicore fibers [67].…”
Section: Discrete Pt-symmetric Oligomersmentioning
confidence: 99%
“…The nonlinear effects in PT-symmetric systems can be utilized for an efficient control of light including all-optical low-threshold switching and unidirectional invisibility [24,56,57]. The possibility to engineer PT-symmetric oligomers, which may include nonlinearity, triggers a broad variety of studies on both the few-site systems and entire PT-symmetric lattices, including onedimensional PT-symmetric dimer [35,58], trimer [58,59], quadrimer [58,60], 2D PT-symmetric plaquettes [60,61], PT-symmetric finite/infinite chains [62][63][64][65], necklaces [66] and multicore fibers [67].…”
Section: Discrete Pt-symmetric Oligomersmentioning
confidence: 99%
“…Thus questions about localization and PT -symmetry breaking in a disordered PT -symmetric system appear moot. 31,32 In this report, we show that the PT -symmetric phase in a disordered system is not always fragile, and that it is protected against random tunneling or on-site potential disorder if the disorder has specific periodicities. We elucidate an underlying symmetry that is critical for the said protection.…”
Section: Introductionmentioning
confidence: 62%
“…We note that in this regime, the intensity I d (k,t) does not reach a steady state value. 4,31,32 Figure 3 (c)-(e) encapsulates the effects of correlated disorder on the disorder-averaged site-and time-dependent intensity I d (k,t). The results are for an N = 39 site lattice with on-site potential disorder with periodicity p = 10, number of disorder realizations M = 10 3 , and an initial state localized at the center of the lattice, k 0 = 20.…”
Section: Disorder Induced Pt Threshold Distribution and Localizationmentioning
confidence: 99%
“…The eigenvalues of matrix C -1 are pairs of two purely real numbers for γ < 0.107, coincide at an EP for γ = 0.107, and then split into a complex conjugate pair ( Figure 6D). This eigenvalue behavior is equivalent to the transition of PT-symmetric Hamiltonians in quantum mechanics from the PT-symmetric phase to the PT-broken phase [11,13,88,89]. The EP of the constitutive matrix C -1 is actually the EP of the S matrix, which leads to the unidirectional reflectionless behavior shown in Figure 6B and C.…”
Section: Unidirectional Reflectionless Propagation In Pt-symmetric Symentioning
confidence: 96%