2009
DOI: 10.1103/physrevb.80.113101
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Parallel-chain optical transmission line for a low-loss ultraconfined light beam

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Cited by 8 publications
(13 citation statements)
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“…This implies that for a correct evaluation of the modal properties and the field distribution generated in this forward-leaky mode regime, the formulas of Eq. operation, whose interesting properties we have already highlighted in details in [12], may lead to ultra-confined low-loss optical guidance in terms of optical nanotransmission-lines. These properties are not only limited to the modes operating near the light line, but they are also valid for higher frequencies and more confined modes.…”
Section: A) Quasi-longitudinal Propagation (Forward Modes)mentioning
confidence: 88%
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“…This implies that for a correct evaluation of the modal properties and the field distribution generated in this forward-leaky mode regime, the formulas of Eq. operation, whose interesting properties we have already highlighted in details in [12], may lead to ultra-confined low-loss optical guidance in terms of optical nanotransmission-lines. These properties are not only limited to the modes operating near the light line, but they are also valid for higher frequencies and more confined modes.…”
Section: A) Quasi-longitudinal Propagation (Forward Modes)mentioning
confidence: 88%
“…This geometry has been preliminarily analyzed in [12] for its longitudinally polarized guided modes, where it was shown that the coupling between the chains, limited in that analysis to its dominant contribution coming from the averaged current density on the chain axes, would generate the splitting of the regular longitudinal mode into two coexisting longitudinal modes, respectively, with symmetric and antisymmetric field distributions. The antisymmetric mode is the one corresponding to transmission-line operation [12], as outlined in the introduction, for which two antiparallel displacement current flows are supported by the parallel chains. A similar modal propagation has been analyzed in [9] for a related distinct geometry, consisting of longitudinal dipoles placed over a perfectly conducting plane.…”
Section: Dispersion Relations For Guided Propagationmentioning
confidence: 99%
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“…A new type of optical waveguide, drastically different from conventional waveguides involving either the Bragg scattering or total internal reflection, is based on the guiding properties of an array of coupled high-Q optical resonators [1]. Recent realizations of such novel waveguides include chains of microresonators or microcavities [2][3][4], magnetoinductive waveguides [5][6][7][8][9][10][11] with magnetic resonators coupled by induced voltages, and chains of metallic nanoparticles with subwavelength localized waves guided due to the excitation of surface plasmon polaritons [12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28]. Very small sizes of plasmonic nanoparticles and the ability of such waveguides to bend without any significant reduction of a signal propagation suggest their use as building blocks for photonic integrated circuits [14].…”
Section: Introductionmentioning
confidence: 99%