Abstract

A curved D-type optical fiber sensor (OFS) combined with a microfluidic chip is proposed. This OFS, based on surface plasmon resonance (SPR) of the Kretchmann’s configuration, is applied as a biosensor to measure the concentrations of different bio-liquids such as ethanol, methanol, and glucose solutions. The SPR phenomenon is attained by using the optical fiber to guide the light source to reach the side-polished, gold-coated region. Integrating this OFS with a polymethylmethacrylate (PMMA)-based microfluidic chip, the SPR spectra for liquids with different refractive indices are recorded. Experimentally, the sensitivity of the current biosensor was calculated to be in the order of 10−5 RIU. This microfluidic chip-integrated OFS could be valuable for monitoring subtle changes in biological samples such as blood sugar, allergen, and biomolecular interactions.

Highlights

  • The surface plasmon resonance (SPR) phenomenon occurs as the consequence of exciting a surface-bound electromagnetic wave at the interface between a metal and a transparent material.Biosensors based on this technique have been designed and constructed for label-free and real-time detection of biomolecular interactions [1,2,3,4,5,6]

  • The results indicated that the optical loss of the Gaussian guided mode could be made very small by tuning the thickness of the dielectric layer and that the refractive-index resolution for aqueous analytes is 1 × 10−4 RIU

  • The results suggest that this microfluidic chip-integrated optical fiber sensor (OFS) can serve as a biosensor for sensitive, label-free, real-time, and in-situ monitoring of biomolecular interactions

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Summary

Introduction

The surface plasmon resonance (SPR) phenomenon occurs as the consequence of exciting a surface-bound electromagnetic wave at the interface between a metal and a transparent material. Biosensors based on this technique have been designed and constructed for label-free and real-time detection of biomolecular interactions [1,2,3,4,5,6]. The grating-coupled SPR takes place when the light diffracted by the grating has different orders with at least one inducing SPR [14,15,16]

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