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Download A Novel Compact Photomic Crystal Fibre Surface Plasmon by Massaro, A.; Akowuah, E.K.; Gorman, T.; Ademgil, H.; Haxha, PDF

By Massaro, A.; Akowuah, E.K.; Gorman, T.; Ademgil, H.; Haxha, S.; Robinson, G.K.; Oliver, J.V

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Additional info for A Novel Compact Photomic Crystal Fibre Surface Plasmon Resonance Biosensor for an Aqueous Environment

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For applications such as 10-Gbit/s-class high-speed modulation1 and free-space interconnect using polarizationdependent optical components, a pinned polarization gives better performance. The competition between the modes with orthogonal polarizations can lead to polarization switching and mode hopping [9,10]. Such behavior is unacceptable for many practical applications such as intra-cavity frequency doubling, where other elements are polarizationdependent. Several approaches for polarization control have been reported based on the introduction of anisotropy to either gain or losses.

Slow down factor increasing as a function of input intensity. 5,7, the input intensity dependent of group delay of the resonance modes during propagation through the 1D-NCCW is obvious. 6 shows group delay for the first and second resonance modes when the input intensity changes from 0 to 6,4 mW/cm2. 05ns. Fig. 6. Group delay versus of input intensity. 38 Photonic Crystals – Innovative Systems, Lasers and Waveguides As mentioned before, photonic structures suffer from fundamental trade off between transmission bandwidth (FWHM of the transmitted resonance modes) and the optical delay, as delay bandwidth product (DBP).

Keeping the defect layer on position 8 (after 8 (AB) groups) we will now vary its thickness to see its influence upon the optical transmission or the frequency of the localized state. a) b) c) d) e) f) Fig. 13. The variation of the thickness of the A type defect layer a) dA=20 mm; b) dA=22 mm; c) dA=24 mm; d) dA=26 mm; e) dA=28 mm; f) the frequency of the localized state vs.

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