1978
DOI: 10.1364/josa.68.001325
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Surface polariton in the ATR angular spectra of a thin iron film bounded by dielectric layers

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1988
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Cited by 21 publications
(8 citation statements)
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“…These propagation lengths are the result of the reduced or increased absorption due to the field distribution in the conducting layer [24]. In 1978 Kovacs demonstrated that high losses in thin slabs of metals is not an impediment for the excitation of long-surface surface modes [25]. This work was extended by Yang and co-workers to non-metallic materials with very large absorption at infrared frequencies [26].…”
Section: Guided Modes Along Absorbing Thin Layersmentioning
confidence: 93%
“…These propagation lengths are the result of the reduced or increased absorption due to the field distribution in the conducting layer [24]. In 1978 Kovacs demonstrated that high losses in thin slabs of metals is not an impediment for the excitation of long-surface surface modes [25]. This work was extended by Yang and co-workers to non-metallic materials with very large absorption at infrared frequencies [26].…”
Section: Guided Modes Along Absorbing Thin Layersmentioning
confidence: 93%
“…A classical waveguide structure is a metal film placed between two dielectric materials with the same permitivity. Two different modes can be excited in such symmetric structure [12] [13]. In another, more widespread asymmetric limiting case, a film of finite thickness is limited on both sides by media with different refractive indices.…”
Section: Introductionmentioning
confidence: 99%
“…These modes arise from the coupling of the evanescently decaying electromagnetic field, as a result of the strong absorption, at the opposite sides of the thin layer. In spite of the similarities between long-range surface plasmon polaritons and long-range guided modes in absorbing thin films there are only a hand-full of articles about the last [12][13][14][15] and, to the best of our knowledge, none about optical sensing.…”
Section: Introductionmentioning
confidence: 99%