Abstract

We review application of microstructured and photonic bandgap fibers for designing resonant optical sensors of changes in the value of analyte refractive index. This research subject has recently invoked much attention due to development of novel fiber types, as well as due to development of techniques for the activation of fiber microstructure with functional materials. Particularly, we consider two sensors types. The first sensor type employs hollow core photonic bandgap fibers where core guided mode is confined in the analyte filled core through resonant effect in the surrounding periodic reflector. The second sensor type employs metalized microstructured or photonic bandgap waveguides and fibers, where core guided mode is phase matched with a plasmon propagating at the fiber/analyte interface. In resonant sensors one typically employs fibers with strongly nonuniform spectral transmission characteristics that are sensitive to changes in the real part of the analyte refractive index. Moreover, if narrow absorption lines are present in the analyte transmission spectrum, due to Kramers-Kronig relation this will also result in strong variation in the real part of the refractive index in the vicinity of an absorption line. Therefore, resonant sensors allow detection of minute changes both in the real part of the analyte refractive index (10−6–10−4 RIU), as well as in the imaginary part of the analyte refractive index in the vicinity of absorption lines. In the following we detail various resonant sensor implementations, modes of operation, as well as analysis of sensitivities for some of the common transduction mechanisms for bio- and chemical sensing applications. Sensor designs considered in this review span spectral operation regions from the visible to terahertz.

Highlights

  • R&D into fiber-optic bio- and chemosensors (FOSs) has made a lot of progress during the last ten years

  • We describe the first resonant sensor type based on hollow core photonic bandgap fibers filled with analyte

  • In what follows we demonstrate an Surface Plasmon Resonance (SPR) sensor using solid core Photonic Bandgap (PBG) Bragg fiber operating at 760 nm, as well as an SPR sensor using honeycomb lattice photonic bandgap fiber operating at 1060 nm

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Summary

Introduction

R&D into fiber-optic bio- and chemosensors (FOSs) has made a lot of progress during the last ten years. In one sensor implementation one can label the target biomolecules with highly absorbing particles of known absorption spectra, such as metal nanoparticles or quantum dots The presence of such particles in the aqueous fiber core can be quantified by detecting appearance of the absorption lines in the fiber transmission spectrum, or through resonant changes in the fiber transmission losses induced by variations in the real part of the core refractive index. Second sensor type considered in this review is operated in the vicinity of a phase matching wavelength between a Gaussian-like core-guided-mode and some other (highorder) mode that shows high sensitivity of its propagation properties to changes in the real part of the analyte refractive index Figure 1(b). Matching between the two modes will be very sensitive to the value of the real part of analyte refractive index

Detection Strategies for Absorption-Based Sensors
Sensing Using Analyte-Filled Hollow Core Photonic Bandgap Fibers
Surface Plasmon Resonance-Based Fiber Sensors
Plasmon-Assisted Sensing Using Solid Core Microstructured Fibers
Plasmon-Assisted Sensing Using Solid Core Photonic Bandgap Fibers
1.48 Plasmon
Plasmon
Section 7.
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