2019
DOI: 10.1364/ol.44.006013
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Kapitza light guiding in photonic mesh lattice

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Cited by 20 publications
(8 citation statements)
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“…pler (θ) as schematically illustrated in Fig. 1(a), similarly to the previous experimental fiber-optical implementations [29]. The length of loops is specially made different, such that the pulses propagating in the long loop are delayed with respect to pulses in the short loop by ∆τ = T long − T short .…”
Section: Introductionmentioning
confidence: 90%
See 1 more Smart Citation
“…pler (θ) as schematically illustrated in Fig. 1(a), similarly to the previous experimental fiber-optical implementations [29]. The length of loops is specially made different, such that the pulses propagating in the long loop are delayed with respect to pulses in the short loop by ∆τ = T long − T short .…”
Section: Introductionmentioning
confidence: 90%
“…Typical pulse durations and roundtrip times exploited in state-of-the-art fiber-optics based SPL are ∆τ ∼ 100 ns and T rt ∼ 20 µs [25]. In these systems, up to M = 200 roundtrips were achieved [29], which is sufficient to create fully connected ONN with N ≤ 100.…”
mentioning
confidence: 99%
“…This effect has been first introduced by Kapitza while studying the dynamics of a forced inverted pendulum, [ 212 ] later on generalized to quantum mechanics [ 211 ] and recently experimentally demonstrated in optics using a fiber‐loop system. [ 213 ]…”
Section: Geometric Phase In Bulk Structuresmentioning
confidence: 99%
“…Various parameters including light intensities and phases (corresponding to the imaginary and real part of potentials), as well as the coupling coefficient of the coupler can be modulated in order to control the flow of light flexibility [21,22]. By engineering these parameters, a number of special phenomena have been investigated in SPLs, diametric drive acceleration [23], time mirror [24] and kapiza light [25]. Naturally, the discretized optical behaviors associated with discrete arrays such as discrete diffraction, Talbot effect [26], Bloch oscillation [27], Anderson localization [28], soliton [29] and other localized states with respect to defect, gauge fields and topological phase transition [30][31][32][33] have been realized in the SPLs under passive or PT -symmetric configurations.…”
Section: Introductionmentioning
confidence: 99%