2012
DOI: 10.1364/ao.51.002752
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On the sensitivity of generic porous optical sensors

Abstract: A porous material was considered as a platform for optical sensing. It was envisaged that the porous material was infiltrated by a fluid that contains an agent to be sensed. Changes in the optical properties of the infiltrated porous material provide the basis for detection of the agent to be sensed. Using a homogenization approach based on the Bruggeman formalism, wherein the infiltrated porous material was regarded as a homogenized composite material, the sensitivity of such a sensor was investigated. For th… Show more

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Cited by 3 publications
(2 citation statements)
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“…But even for values of ǫ hcm well away from the immediate vicinity of Re ǫ hcm ≈ 0, the magnitudes of the sensitivity measure dθ c /dn b presented in Figs. 5, 6, 7, 8 and 10 compare favourably to sensitivities associated with optical sensing approaches based on surface-plasmon-polariton waves [33,34,35,36,37], Voigt waves [38,39], as well as generic porous dielectric materials [40]. We note that the issue of relatively large losses that arises in the parameter regime where Re ǫ hcm ≈ 0 could, in principle, be addressed by the use of active component materials [41].…”
Section: Discussionmentioning
confidence: 80%
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“…But even for values of ǫ hcm well away from the immediate vicinity of Re ǫ hcm ≈ 0, the magnitudes of the sensitivity measure dθ c /dn b presented in Figs. 5, 6, 7, 8 and 10 compare favourably to sensitivities associated with optical sensing approaches based on surface-plasmon-polariton waves [33,34,35,36,37], Voigt waves [38,39], as well as generic porous dielectric materials [40]. We note that the issue of relatively large losses that arises in the parameter regime where Re ǫ hcm ≈ 0 could, in principle, be addressed by the use of active component materials [41].…”
Section: Discussionmentioning
confidence: 80%
“…Indeed, in the limit ǫ hcm → 0 − , the critical angle θ c → π/2 and the derivative dθ c /dn b becomes unbounded. However, [33,34,35,36,37], Voigt waves [38,39], as well as generic porous dielectric materials [40]. We note that the issue of relatively large losses that arises in the parameter regime where Re ǫ hcm ≈ 0 could, in principle, be addressed by the use of active component materials [41].…”
Section: Discussionmentioning
confidence: 98%