We report the application of the analytical and finite element methods to the analysis of the sensing performance for the Bragg fiber-based plasmonic sensors having four layers. The advantages of an optical fiber with four (SiO2, GaP, gold, and H2O) layers are a very large value of the am- plitude sensitivity (3708.8 refractive index units (RIU)−1), large values of the loss (3091.0 dB/cm) and the power fraction P (0.36) at the loss matching point for the core mode in H2O, a small value of the full width at half maximum (19.4 nm), a smaller value (2.1 nm) of the difference Δλ between maximal amplitude sensitivity and resonant wavelengths, and a sym- metric line shape of the wavelength-dependent loss but a small spectral sensitivity (3236 nmRIU−1). A modification in the geometry of the fiber produces a significant change in the sensitivity and in the propagation parameters of the device. Thus, the advantages of another optical fiber with four layers are a very large value of spectral sensitivity ( nmRIU−1), large values of the amplitude sensitivity (2084.4 RIU−1), and the loss (3214.5 dB/cm) and the power fraction P (0.35), but the difference Δλ is large (8.6 nm) and the line shape for the wavelength dependence of the imaginary part of the effective index is asymmetric.

Sensing Performance of the Bragg Fiber- Based Plasmonic Sensors with Four Layers / Popescu, V. A.; Puscas, N. N.; Perrone, Guido. - In: PLASMONICS. - ISSN 1557-1955. - STAMPA. - (2016), pp. 1-7. [10.1007/s1146801501581]

Sensing Performance of the Bragg Fiber- Based Plasmonic Sensors with Four Layers

PERRONE, Guido
2016

Abstract

We report the application of the analytical and finite element methods to the analysis of the sensing performance for the Bragg fiber-based plasmonic sensors having four layers. The advantages of an optical fiber with four (SiO2, GaP, gold, and H2O) layers are a very large value of the am- plitude sensitivity (3708.8 refractive index units (RIU)−1), large values of the loss (3091.0 dB/cm) and the power fraction P (0.36) at the loss matching point for the core mode in H2O, a small value of the full width at half maximum (19.4 nm), a smaller value (2.1 nm) of the difference Δλ between maximal amplitude sensitivity and resonant wavelengths, and a sym- metric line shape of the wavelength-dependent loss but a small spectral sensitivity (3236 nmRIU−1). A modification in the geometry of the fiber produces a significant change in the sensitivity and in the propagation parameters of the device. Thus, the advantages of another optical fiber with four layers are a very large value of spectral sensitivity ( nmRIU−1), large values of the amplitude sensitivity (2084.4 RIU−1), and the loss (3214.5 dB/cm) and the power fraction P (0.35), but the difference Δλ is large (8.6 nm) and the line shape for the wavelength dependence of the imaginary part of the effective index is asymmetric.
2016
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11583/2627060
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