2008
DOI: 10.1080/09500340802271250
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Field profiles of coupled surface plasmon-polaritons

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Cited by 34 publications
(34 citation statements)
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“…The optical excitation of the LRSPP was applied to increase the sensitivity of refractive index sensing in surface plasmon resonance (SPR) sensors [12]. In a metal-insulator-metal (MIM) structure consisting of an insulator layer sandwiched by metals, the coupling between two SPPs at the two I/M interfaces generates also the S-SPP and AS-SPP modes [7][8][9][13][14][15][16][17]. The AS-SPP mode in the MIM structue is also a long-range mode.…”
Section: Introductionmentioning
confidence: 99%
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“…The optical excitation of the LRSPP was applied to increase the sensitivity of refractive index sensing in surface plasmon resonance (SPR) sensors [12]. In a metal-insulator-metal (MIM) structure consisting of an insulator layer sandwiched by metals, the coupling between two SPPs at the two I/M interfaces generates also the S-SPP and AS-SPP modes [7][8][9][13][14][15][16][17]. The AS-SPP mode in the MIM structue is also a long-range mode.…”
Section: Introductionmentioning
confidence: 99%
“…The electromagnetic modes supported by the MIM structure have long been studied theoretically and experimentally [7][8][9][13][14][15][16][17][18][19][20]. In addition to the S-SPP and AS-SPP that arise from the coupling of two degenerate SPP modes, the MIM structure can support transverse electric (TE) modes analogous to those supported by Fabry-Pérot cavities [34].…”
Section: Introductionmentioning
confidence: 99%
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“…42 Losses due to surface roughness are likely to be more apparent when a surface mode is excited (as here) then for normal incindence illumination (as for our parameter retrieval procedure). We have also calculated 43 and plotted the magnetic component of the p-polarised optical field through the sample for the same incident wavelength and angle in Figure 4b. In this figure two features are apparent: first, going from the prism/TDBC:PVA interface into the TDBC:PVA film the field decays with distance -this is expected for an absorbing film; second, the field rises again towards the TDBC:PVA/air interface -indeed, the field decays on either side of the TDBC:PVA interface, just as expected for a surface mode.…”
mentioning
confidence: 99%
“…The terms long-range and short-range surface modes arise from the respective long and short propagation lengths of these modes compared to the propagation of SPPs on single interfaces. 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].…”
Section: Guided Modes Along Absorbing Thin Layersmentioning
confidence: 99%