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Polymer Fiber Optic Sensors A Mini Review of their Synthesis and Applications | OMICS International
ISSN: 2155-6210
Journal of Biosensors & Bioelectronics

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Polymer Fiber Optic Sensors A Mini Review of their Synthesis and Applications

Yan Jin and Anthony M Granville*

Centre for Advanced Macromolecular Design, School of Chemical Engineering, University of New South Wales, Sydney, Australia

*Corresponding Author:
Anthony M Granville
Centre for Advanced Macromolecular Design
School of Chemical Engineering
University of New South Wales
Sydney, Australia
Tel: +61 2 9385 5745
Fax: +61 2 9385 5966
E-mail: [email protected]

Received Date: November 17, 2015; Accepted Date: December 10, 2015; Published Date: January 01, 2016

Citation: Jin Y, Granville AM (2016) Polymer Fiber Optic Sensors – A Mini Review of their Synthesis and Applications. J Biosens Bioelectron 7:194. doi:10.4172/2155-6210.1000194

Copyright: © 2016 Jin Y, et al. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.

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Fiber optic sensors (FOSs) are optical fiber based sensing devices that have been widely used to detect physical, chemical and biological parameters. Polymer optical fibers (POFs), an important type of optical fibers, have been stifled their talents in the field of optical sensing due to the overwhelming popularity of glass optical fibers (GOFs). The unique physical and chemical properties of POFs start attracting interests to be utilized in the fabrication of high performance sensors in recent years. This article reviews the recent progress of POFs based FOSs. In particular, the article will focus on novel techniques implemented on the POF sensor fabrication, including monolayer graphene, evanescent wave absorption, localized surface plasmon resonance and fiber Bragg grating.


Polymer fiber optic sensor; Evanescent wave; Localized surface plasmon resonance; Fiber Bragg gratings; Microstructured polymer optical fiber


Although it is an essential part of modern communication, the light guiding capabilities of optical fibers were first demonstrated in the early 1840 s by Daniel Colladon and Jacques Babinet who showed that light can be guided through the glass fiber by the total internal reflection (TIR) at the fiber’s inner surface [1]. Fiber optic sensors (FOSs) operate on the principle that the light transmitted through the fiber core can be affected by its surrounding environment [2]. Over the years, a range of FOSs have been developed to measure a variety of parameters, including physical (displacement, stress and wind speed) [3-5], chemical (pH, organic and inorganic compound concentrations) and biological parameters (blood glucose and oxygen concentrations) [6,7]. To date, FOSs are frequently developed using glass optical fibers (GOFs) due to their low attenuation of light signals and commercial availability [8]. However, the limitations for developing sensors from GOFs have usually, but not exclusively, been due to the demanding procedures for fiber processing rather than their performance [9]. On the other hand, polymer optical fibers (POFs), with structure and light guiding properties comparable to GOFs, are receiving increased attention from researchers due to their high flexibility and ease of handling [2,6,10]. In particular, the surface properties of POFs can be easily manipulated by simple and wide-ranging chemistry techniques to achieve the desired sensing properties.

The relevant theories of fiber optical sensors have been thoroughly explained by Udd [11] and López-Higuera [12]. Early reviews of polymer optical fibers sensors are included in some general reviews of fiber optic sensors, including Grattan [13], Zubia [2], Bartlett [14] and Leung [15]. Recently, more specific reviews on polymer fiber based optic sensors are given by Peters [16] and Bilro [8]. This paper presents a brief review of the recent developments in POF sensors and their applications, specifically, the most common fabrication techniques and sensing mechanisms will be demonstrated and discussed.

Polymer optical fibers

POFs were developed nearly at the same time as the GOFs, but they have received far less attention compared to GOFs. The relatively high signal attenuation of POFs makes them unsuitable for long-haul communications. However, their ease of handling, greater flexibility and high robustness make POFs ideal for short-haul communications and sensing applications [2]. Since the invention of POFs, continuous efforts have been devoted to POFs technologies and developments to improve its light guiding properties. Several types of POFs have been developed thus far, including single/multi-mode POF (SM/MM-POF), step-index POF (SI-POF), graded-index POF (GI-POF), fluorinated POF (CYTOP) and the latest multi-core POF [2,17].

The structure of a common MM-SI POF consists of three layers: core, cladding and jacket (Figure 1). The refractive index of the cladding (ncl) is designed to be lower than that of the core (nco), so it can facilitate TIR in the fiber core. Several core materials have been utilized for POFs such as poly (methyl methacrylate) (PMMA), polystyrene (PS) and polycarbonate (PC). Each of the core materials has its own unique characteristics and applications. For example, PMMA POFs have relatively high transparency in visible and near-infrared regions and hence they are the most common POFs on the market, while PC POFs have better heat resistance compared to PMMA POFs and hence they can be used to fabricate sensors in a high temperature environment [2]. The jacket is a plastic layer on the cladding which provides protection for the fiber from chemical decomposition and mechanical damages. It is worth noting that, in some cases such as POFs for sensing applications, uncladded POFs (without the cladding and the jacket) are frequently used as the sensing events occur on the surface of the fiber core.


Figure 1: The structure of a modern optical fiber [2]. Reprinted with permission from Elsevier, copyright 2001.

Over the years, technological advances have allowed the production of high-quality POFs at lower cost. Currently, two main techniques have been widely adopted for producing SM/MM-SI POFs: drawing process and extrusion process [18].

Drawing process

Garvey et al. described the general procedures for the POF drawing process [19]. First, a cylindrical shape of polymer preform is obtained with a typical diameter of 0.5-1 m. The preform obtained has the same index profile as the fiber core being drawn. Next, the preform is transferred to a fiber drawing tower, where it is drawn into a smaller fiber with a predetermined diameter. Figure 2 illustrates a typical drawing tower: a stepper motor holds the preform vertically and feeds it into an oven. The optimal heating condition varies with the preform material and is usually determined empirically. In the oven, the polymer becomes soft and forms a neck-down region. The fiber below the neck-down region can be extruded into a smaller fiber, while the diameter of a POF is controlled by a three-pulley stress gauge system (not shown in the figure) [18]. The fiber exits the tension gauge system by a take-up spool and ready for further processing. The drawing process is a rather simple operation and can be used for production of various kinds of POFs using the corresponding polymer performs that are commercially available. The main problem associated with this process arises from variations of drawing conditions during the manufacturing process that could change the index of fiber from one section to another [19].


Figure 2: Schematic diagram of a POF drawing tower.

Extrusion process

Compared to the drawing process, the extrusion process produces POFs directly from monomers either continuously or in batches. The extrusion process can be performed under air or in a closed environment (thrust extrusion) [17]. Compared to the open air extrusion process, thrust extrusion prevents any impurities which influence the optical properties of the final POFs.

Figure 3 shows a schematic diagram of a typical thrust extrusion process for producing PMMA POFs [20]. At the beginning of the process, monomer, initiators and other necessary substances are distilled into a closed reactor under vacuum to minimize the amount of air dissolved in the system. The polymerization is carried out at 135°C for 12 h and then raised to 180°C for another 12 h to achieve a high conversion of the monomer [18]. After the polymerization process is completed, nitrogen is used to generate high pressure in the reactor to push the melted polymer through a small nozzle, producing the desired fibers. The remaining monomers can be evaporated and recovered back into the feedstock. Although the thrust extrusion process produces higher quality POFs than that produced from the drawing process, the higher requirements for equipment and operations limit its applications to mainly industrial scale POF productions.


Figure 3: Schematic diagram of a PMMA POF extrusion apparatus [20]. Reprinted with permission from AIP Publishing LLC, copyright 1982.

Polymeric optical fiber sensors

Fiber optic sensors can be classified into several categories depends on their configurations, working mechanisms and applications. One of the generally accepted classifications is extrinsic and intrinsic sensors (Figure 4). In an extrinsic sensor, the optical signal leaves the waveguide first, entering a sensing region and then re-enters the second waveguide. On the other hand, for an intrinsic sensor, the optical signal does not leave the waveguide, it is either reflected back to the entering side (reflection system) or transmitted to the other side of the waveguide (transmission system). For intrinsic sensors, a reflection system utilizes absorption, fluorescence, light scattering, refractive index and intensity variations etc. to detect target parameters. On the other hand, transmission systems can further take advantage of evanescent wave absorption to monitor changes occurring on the surface of the fiber. Since transmission systems have the capability to fully explore the large side-surface area of the optical fibers, thus the following review will focus on intrinsic sensors.


Figure 4: (a) Extrinsic system, (b) intrinsic-reflection system, (c) intrinsictransmission system.

Intrinsic-reflection POF sensors

Intrinsic-reflection systems are the conventional configuration for the fabrication of fiber optic sensors. Among the intrinsic-reflection systems reported to date, the majority employ indicators at the fiber ends which respond to the parameters to be detected. Indicators employed in intrinsic-reflection POF sensors are frequently doped in a thin film and subsequently dip-coated (e.g. sol-gel technique) or physically attached onto the fiber end. Thin film techniques have been well investigated and developed for the fabrication of GOF sensors during the last few decades and these technologies have been successfully transferred to fabricate POF sensors.

Utilizing sol-gel technology to create a thin porous film incorporating sensing elements for optical sensors, especially biosensors, has attracted considerable interest. Thin films on the fiber ends with a desired layer thickness can be easily fabricated through a simple process which includes spin-coating, dip-coating and spraycoating [21]. By carefully tailing the supporting materials, fabrication process and layer configuration, the thin film can achieve a high compatibility with biological molecules, such as enzymes, DNA and even whole cells. The relevant theory of sol-gel techniques has been thoroughly discussed by Jerónimo and MacCraith [22].

Fiber optic sensor for pH sensing and imaging is the field where sogel techniques have been most frequently implemented. This is due to the convenience of incorporating pH indicators into the sol-gel matrix, which, compared to conventional pH sensors, offers several advantages such as fast response, high resolution, low cost and immunization of EMI. Fabbri and Rovati reported a disposable pH sensor based on an organic-inorganic hybrid matrix–ORMOSILs (organically modified silicates) that were doped with a pH sensitive dye [23]. Polyethylene oxide (PO) was used as the organic fraction of the matrix, which allows for good adhesion between the POF and the porous matrix. It also can be used to tune the diffusion rate of the analyte inside the porous matrix. The inorganic fraction of the matrix–silica glass (prepared from tetraethyl orthosilane, TEOS)–enhances the ductility and permeability of the matrix. The hybrid matrix was obtained from a typical sol-gel technique and then dip-coated on the tip of a PMMA fiber. The sensing range was found to be pH 4-10 with less than 1 second response time. Later on, Schryy et al. adopted a similar strategy using TEOS and methyltriethoxysilane (MTES) to prepare an organic-inorganic matrix that supports bromophenol blue (BB) to monitor pH in biological fluids [24]. The optimum amount of organic compound–MTES was found to be 50 wt% which reduced dye leaching in phosphate buffered saline (PBS) within 20% for the duration of 2 months. The fabricated sensor showed good sensitivity in the range of pH 5-8, and temperature independence within 20 to 25°C. Furthermore, in vitro tests in human serum showed reversible pH monitoring between pH 5-8 with 0.2 pH unit resolutions.

Along with pH sensing, chemical aerosol detection has been performed by Kulkarni et al. testing the possibility of using two types of thin film configurations, TEOS and TEOS doped with thylmol blue (TB) [25]. By utilizing a typical sol-gel technique, a thin layer of TEOS was doped onto the end surface of a POF. The fabricated POF sensor was equipped with 4 types of light sources: UV (λ = 340 nm), blue (λ = 440 nm), red (λ = 660 nm) and infrared (λ = 940 nm), which were used to detect black carbon (BC) and sulfate-(NH4)2SO4 aerosols. The preliminary testing results showed that TB doped films demonstrated a better sensitivity than pure TEOS films and blue light sources led to a more significant intensity change due to the stronger absorption by aerosols: 2.22% for sulfate and 2.16% for BC. The authors also pointed out that, by carefully controlling the thickness of thin film, the sensitivity could be further improved.

Portable, low cost and fast detection of nitro aromatic explosives, such as trinitrotoluene (TNT) and trinitrophenol (TNP) remain a critical importance for safety reasons. The discovery of fluorescein conjugated-poly(2-methoxy-(2’-ethylhexloxy)-p-phenylene-vinylene) (MEH-PPV) enables fast identification of these explosives due to its fluorescence quenching effect when in contact with nitro aromatic compounds [26]. Chu et al. reported a TNT POF sensor by dip coating MEH-PPV on a coil-shaped PMMA fiber [27]. It was discovered that better sensitivity could be achieved by measuring the fluorescent life time rather than the intensity, while the sensitivity was also improved for the fibers with a smaller coil. However, the sensor’s lowest detection limit (1-15 ng·mL-1) was extrapolated from the sensor’s response curve, which needs to be verified by experimental tests. Irreversible quenching of using MEH–PPV by TNT is one of the main drawbacks of the sensor, meaning that it is not suitable for in vitro measurements.

Graphene, the two-dimensional nanomaterial, is a good candidate to be used as the sensing elements in the application of fiber optic sensing technologies. The properties and production technique of graphene have been reported in some comprehensive reviews [28-30]. The characteristics of ultra-low thickness, high permeability, good optical transparency as well as chemical inertness make graphene films ideal carriers for binding of transducer reagents in integrated biochemical transducer fiber optic systems [31-34]. Currently, the application of graphene in FOSs has been mostly focused on GOFs, while a limited number of POF based FOSs has been reported [35-37].

Kulkarni et al. first reported a simple strategy to transfer large area graphene films onto the distal end surface of PMMA fibers by direct deposition of preformed graphene films synthesized via a chemical vapor deposition (CVD) technique [36]. This technique was later implemented by the same research group who designed a volatile organic compounds (VOCs) sensor via depositing a monolayer of graphene or graphene oxide onto the distal end of a PMMA fiber [37,38]. The intensity of light reflected from the deposited thin film will change accordingly when the film absorbs VOCs present in the atmosphere. Recently, POFs with their claddings replaced with graphene films have demonstrated the capability to detect biomolecules in aqueous mediums by monitoring the shift of surface plasmon resonance (SPR) [35].

Intrinsic-transmission POF sensors

The highly restricted sensing area (fiber distal-end) of intrinsicreflection systems significantly hinders the efforts to improve their sensing performance. Meanwhile, the emergence of new types of POFs (e.g. microstructured POFs and fiber Bragg gratings) and detection mechanisms (e.g. evanescent wave absorption and localized surface plasmon resonance) provide intrinsic-transmission systems with much greater potentials due to their detection diversity and sensitivity. For that reason, intrinsic-transmission systems have dominated the research of FOSs in recent years.

Evanescent wave absorption (EWA) POF sensors have been receiving increasing attention from researchers due to their potential medical applications in detecting biomolecules [39-41]. When light is transmitted through the fiber, it undergoes total internal reflection on the inner surface of the fiber core. This internal reflection gives rise to the standing wave at the interface along the axis of the fiber due to the interference between incident and reflected beams. Since the amplitude of the standing wave does not decay to zero at the boundary between the fiber core and the surrounding medium, it penetrates a short distance into the surroundings. This ‘’leakage’’ of light from the wave guide is defined as an evanescent wave (EW). The intensity of the EW present on the fiber surface can be expressed in the following equation [42]:

Equation (1)

Where, E0 is the power of light coupled into the fiber, E is the power of the EW, δ depicts the distance from the interface and dp stands for the penetration depth of the EW where the amplitude of the intensity fall to 1/e its value at the interface [42].

Equation (2)

Penetration depth-dp depends on several parameters: the wavelength of coupled light (λ), the refractive indexes of core (nco), surrounding medium (ncl), and incident angle (θ) between the ray and the normal interface.

The EW interacts with analytes in the vicinity of fiber surface via absorption of EW at certain wavelengths or emission of light after EWA (luminescence) (Figure 5) [17]. By analyzing the output light spectrum, the fingerprints of solids, liquids and gases that present on the surface can be obtained.


Figure 5: Operating principles of the surface modified POF sensors.

In most cases, the target analyte cannot be detected directly because its interaction with the EW does not always lead to a detectable spectra change (e.g. weak absorption of EW). The common solution is to use indicators that can interact with analytes, producing a certain detectable change in the micro-environment of the fiber surface [43]. One of the most commonly employed indicators is metal nanoparticles of noble metals. When excited by an EW, the nanoparticles immobilized on the fiber surface will be excited to trigger a well-known optical phenomenon called localized surface plasmon resonance (LSPR) which exhibits ultrahigh sensitivity towards the variation of refractive index in the vicinity of the particle surface [44,45]. LSPR effect and the corresponding LSPR POF sensors lay the foundation for the research project reported in this thesis hence these topics will be further explored individually in subsequent sections.

One of the basic applications of tapered EWA POF sensors is to detect the salinity of salt water as the increase of medium refractive index would result in the reduction of the light intensity transmitted through the fiber [46]. However, the sensor response to bulk refractive index variations caused by salinity changes due to the unspecific detection mechanism. The EWA salinity POF sensor does not provide significant detection improvement over conventional electrical sensors [47].

More advanced development of EWA POF sensors involves the implementation of an indicator. Pulido et al. reported a EWA POF oxygen sensor based on the fluorescence-quenching effect of oxygen on cationic ruthenium complexes [48]. Tris (2,2’-bipyridyl) dichlororuthenium(II) hexahydrate was first dissolved in the solvent of acetone and water, followed by immersing the tapered section of PMMA POF in the solution for a short period of time. Due to the partial surface dissolution of PMMA POF caused by acetone, the ruthenium complex was able to diffuse into the upper layers of the PMMA POF and being trapped. The reported sensor showed linear responses to oxygen concentration from 0-100 vol% both in terms of fluorescenceintensity and fluorescence lifetime. However, the immersion time of PMMA POFs in the acetone and water mixture has to be carefully controlled as the mechanical stability of PMMA POFs degraded rapidly in the solution. A sol-gel technique was also employed to anchor ruthenium complexes onto a U-shape polymer fiber for the fabrication of a dissolved oxygen sensor [49]. Ruthenium (II) chloride was incorporated into a sol-gel prepared from TEOS and MTEOS and then dip-coated onto a U-shape de-cladded PMMA fiber. However, non-linear responses were observed for both fluorescence intensities and lifetimes against oxygen concentrations. The authors proposed a two-layer model to explain this non-linearity: the sensing film consists of two layers, the outer layer contacts the dissolved oxygen directly while the inner layer does not. With the proposed two-layer model and the previously reported dynamic/static quencher model combined [50], the new model is more comprehensive in explaining the non-linear behavior of the experimental data.

A tapered EWA POF biosensor was report by da Silva et al. for the detection of red blood cells (RBC) and bacterium Escherichia coli [51]. A small region of a PMMA POF (1 mm in diameter) was heated above its glass transition temperature and pulled to form a tapered section (0.35 mm in diameter) with a biconic format. Then, hexamethylene diamine (HMDA) and glutaraldehyde were applied to the tapered region followed by protein A for the subsequent immobilization of anti-RBC and anti-E.coli. An LED light source (540 nm) was irradiated into the fiber which was further split into two channels: one entered the sensing fiber and the other one entered the reference fiber. The testing results were positive for RBC at concentrations of 108 colony forming units·mL-1 (CFU·mL-1) while failed for anti-E.coli due to the weak absorbance at 540 nm. However, E.coli was successfully detected at a minimum concentration of 104 CFU·mL-1 by switching the emission source to longer wavelengths (880 nm) due to the stronger EW intensity presented on the fiber surface [52]. Although the sensitivity of the reported EWA POF biosensor was considerably lower than the methods currently available on the market (e.g. polymerase chain reaction technology can achieve <102 CFU·mL-1) [53], the continuous improvements of the EWA POF biosensor would certainly make it more competitive in the near future.

Intrinsic-transmission POF sensors using Fiber Bragg Gratings

Fiber Bragg grating (FBG) sensors are a type of wavelength– encoded sensor. FBG-based sensing devices directly transform sensed parameters into shifts of optical wavelengths, which have the advantage of minimal influence caused by extraneous optical power variations. According to the theory of Fresnel reflection, the light wave can reflect and refract at the interface of the two mediums which have different refractive indices. By varying the refractive index of the fiber core periodically (using laser or UV light), FBGs can act as a wavelengthspecific dielectric mirror that reflect certain wavelengths of the input light and transmit through the rest of the wavelengths [54]. Figure 6 illustrates a uniform positive index change FBG which is the simplest form of FBG that is employed most frequently in the FBG sensor fabrication.

Equation (3)


Figure 6: Uniform positive index change FBG.

The light guiding properties of a FBG is governed by Equation 3 [54], where ne is the effective refractive index of the grating in the fiber core, λB is the Bragg wavelength and Λ is the grating period. The sensing capabilities of FBG sensors are determined by ne and λB. When external stimuli are applied to a FBG sensor, such as strain, pressure, humidity and temperature variations, ne and Λ would change accordingly and result in the shift of λB. Therefore, all FBG sensors are intrinsically sensitive to the aforementioned stimuli [55]. Recently, extension of the sensing capability of FBG sensors to detect biological agents has been reported by modifying the fiber grating surface which induces binding of biological analytes. Once analytes bind onto the fiber grating surface, they change the surface strain of the fiber and result in a shift of the Bragg wavelengths [56-58]. However, due to the interference caused by the surrounding environment, such as humidity and temperature variations, the performance of FBG biosensors is inferior compared to other types of fiber optic biosensors and a major breakthrough is still required. The following section will mainly focus on the well-developed FBG sensors to detect physical parameters.

Using POFs to fabricate FBG sensors offers several advantages over GOFs. The lower Young’s modulus of POFs leads to a higher failure strain which results in an improved sensitivity and detection range. Additionally, by taking advantages of the high flexibility and easy processing of POFs, asymmetric structure of polymer based FBG sensors can be fabricated to achieve certain functionalities. The first polymer FBG was fabricated by Xiong et al. [59]. FBG was incorporated into a SM PMMA POF using a pulse laser beam operating at 248 nm. After that, several polymer FBGs were developed with different Bragg wavelengths, dopants and fiber geometries [60-63]. Recently, more attention has been drawn to inscribing Bragg gratings into microstructured polymer optical fibers (mPOFs) due to their superior properties, which will be discussed in the following section [64-67].

Strain, temperature and humidity measurements are one of the most common fields in which polymer FBG sensors have so far been implemented. Luo et al. evaluated the performance of a polymer FBG when measuring stress and strain [68]. The authors inscribed gratings into a SI-MM POF with the core doped with benzyl dimethyl ketal (BDK) to enhance the photosensitivity. A 355 nm frequency-tripled Nd: YAG laser was used to inscribe gratings into POFs with Bragg wavelength of 1570 nm. The maximum sensitivity of axial stress was determined to be 472 pm·MPa-1 under 9.59 MPa stress, while the sensitivity of axial strain was comparable to GOF based FBG sensors (1.18 pm·μ?-1). Later on, the same research group extended the use of the polymer FBG sensor in measuring temperature [69]. Both theoretical simulation and experimentation showed that the MM polymer FBG sensor can achieve a higher sensitivity by an order of magnitude than their glass FBG counterparts.

Besides the commonly adopted techniques that use laser or ion beams to inscribe Bragg gratings into POFs or GOFs, Gu et al. demonstrated a high strain sensitivity polymer micro/nanofiber Bragg gratings (MNFBGs) employing a low cost nanoimprinting approach [70]. Similar to the technique adopted in the fabrication of gratings in planar waveguides, they used a standard plane reflection grating as a mold to imprint gratings on a POF when it was heated above its glass transition temperature. The axial strain sensitivity of the fabricated FBG sensor was determined to be -2.5 pm·μ?-1 which is almost doubled when compared to common polymer FBG strain sensors [68]. One apparent difference of this FBG sensor is the blue shift of the Bragg wavelength upon applying strain, in contrast to the response of FBG sensors fabricated using laser or ion beams. The authors believe this contradiction was resulted from a large photo-elastic effect when applying strain, while the red shifts from conventional FBG sensors were caused by the elongation of the fibers.

The realization of multiplex sensing in FBG sensors, especially in measuring physical parameters, is much easier than other FOSs. Bragg gratings were reported by writing into an eccentric core polymer optical fiber (ecPOF) to fabricate a strain, bend and temperature sensor [71]. Compared to concentric polymer fibers, ecPOF has characteristics of directional bend sensitivity and wide curvature measurement range. The POF used for sensor fabrication was a SI-SM PMMA fiber with a core offset of 24 μm from the neutral axis, the diameters of the core and the cladding was 8.1 μm and 230 μm, respectively. The Bragg grating was inscribed into ecPOF via a common scanning phase mask technique using a CW He-Cd laser operated at 325 nm. The bend experiments were carried out for four orientations individually. For each rotational orientation, the Bragg peak shift was monitored for curvatures ranging from 0 to 22.7 m-1. The maximum sensitivities were found to be 63.3 pm·m-1 at 180° orientation (extension) and -56.4 pm·m-1 at 0° orientation (compression). The strain and temperature tests showed the FBG in an ecPOF had a maximum sensitivity of 1.13 pm·μ?-1 and -50.1 pm·°C-1.

Polymer FBG sensors can respond to the humidity variations in the surrounding environment when water from the atmosphere diffuses into the fiber. Zhang et al. compared the performance of POF and GOF based FBGs in measuring humidity and temperature [72]. FBG was inscribed into a MM PMMA POF using He-Cd laser at 325 nm and into a SM GOF using Argon laser at 244 nm. The PMMA POF had a core diameter of 10 μm and a cladding thickness of 130 μm. At a constant temperature of 25°C, the POFs showed a linear response to the relative humidity in the range of 50–95% with a sensitivity of 35.2 pm·%-1, while for the GOFs, a sensitivity of only 0.28 pm·%-1 was achieved. At constant humidity, the POFs still performed better than GOFs in measuring temperature with a sensitivity of -55 pm·°C-1 compared to 13.9 pm·°C-1 for the GOFs. Hysteresis is the major problem using FBG PMMA POFs in the monitoring of relative humidity–up to 30 minutes response time was required to reach the full response. This can be partially resolved by etching a fiber’s cladding to speed up the diffusion of the water into the core [73].

The drawback for polymer FBG sensors is also obvious, the commonly used PMMA POF can only absorb moisture up to 0.3 wt% [74]. When using polymer FBG sensors to monitor temperature, strain or stress in the air, the measurements need to be calibrated against the relative humidity at same time. This cross-sensitivity imposes a significant drawback to the implementation of polymer FBG sensors in the field [75,76]. Recently, a new type of polymer material–cyclic olefin copolymers (TOPAS®) – has drawn considerable attention from researchers due to its low affinity towards water and chemical inert nature [74]. High quality Bragg gratings were first successfully inscribed into TOPAS® mPOF by Johnson et al. [77]. By using a He-Cd laser, FBG was incorporated into a SM TOPAS mPOF with a Bragg wavelength of 1567.7 nm. When the TOPAS® mPOF based FBG sensor was examined at an environment with a constant relative humidity of 55%, the sensor showed a linear response to the temperature variation from 20 to 35°C and a sensitivity of -36.5 pm·°C-1. However, the authors also pointed out that one of the limitations of using TOPAS® is its low glass transition temperature (78°C), 30°C less than PMMA. Yuan et al. [78], from the same research group, examined the influence of humidity on TOPAS® mPOF based FBG sensor in measuring strain and temperature. In addition to having the operating wavelength set at the conventional Bragg wavelength of 1568 nm, the authors also fabricated a FBG that operated between 800–900 nm to reduce the power loss in the fiber. At 870 nm, the sensitivity of the TOPAS® mPOF FBG sensor was determined to be 0.64 pm·μp-1 (up to 2.17% strain) and -78 pm·°C-1 (23°C to 32.6°C). The strain sensitivity is similar to the PMMA based FBG sensor reported previously [64,65], while the sensitivity in temperature was doubled [77], which was due to the smaller diameter of the fiber used. The humidity tests illustrated that the TOPAS® FBG sensor responded linearly to the humidity change. For the TOPAS® FBG sensor operated at 849 nm, sensitivity was observed to peak at 0.7 pm·%-1 when decreased the relative humidity from 90% to 50%. For the TOPAS® FBG sensor operated at the Bragg wavelength of 1568 nm, maximum of sensitivity of -0.59 pm·%-1 was observed when the relative humidity was increased from 30% to 90%.

A polymer FBG strain sensor can be easily converted into an accelerometer. Stefani et al. developed an accelerometer using a SM PMMA mPOF based FBG sensor [79]. FBG was incorporated into a mPOF with Bragg wavelengths of 1550 nm and 850 nm using a phase mask technique. Then, an accelerometer prototype was prepared by using a fork-shaped mechanical transducer to convert the acceleration into strain through elongation of the fiber caused by acceleration. The accelerometer showed a frequency response up to 1 kHz and the resonance frequency was found to be 3 kHz. At a resonance wavelength of 1550 nm, a linear sensitivity of 19 pm·g-1 up to 15 g of acceleration was achieved; while for the 850 nm mPOF, the sensitivity was found to be 7.6 pm·g-1. Comparing the mPOF and GOF FBG accelerometers fabricated by the same method showed that the mPOF sensor achieved more than four times greater sensitivity over its counterpart at both Bragg wavelengths.

Microstructured POF sensors

Microstructured optical fibers (MOFs), also as known as photonic crystal fibers (PCFs), are a newly emerging type of waveguide that can guide the light through hollow cores running longitudinally along the fiber. The MOFs can be divided into several categories based on their geometries and light guiding mechanisms, including photonicband gap fiber, holey fiber, hole-assisted fiber and Bragg fiber [80,81]. Employing MOFs to develop optic sensors have several prominent advantages over conventional solid core fibers. Indicators or sensing layers adopted in the hollow cores inside the MOFs provide significantly more sensing areas and stronger interactions with the transmitted light waves than the conventional fibers. The location of sensing elements is isolated from the surrounding environment and hence minimizes any undesirable external interference. mPOFs offer additional benefits over their glass counterparts due to their ease and versatility of fabrication techniques and intrinsic tailorability of the polymers [82,83].

Li and Wang et al. reported a mPOF sensor using Rhodamine 6G (Rh 6G) as the indicator for the detection of hydrogen peroxide and nitrites [84,85]. Li and Wang first used a titanium oxide film as the carrier for Rh 6G to detect the hydrogen peroxide [84]. The acidic solution containing tetrabutyl titanate, ethanol and Rh 6G was drawn into the hollow holes to form a three-dimensional network of titanium dioxide with entrapped Rh 6G. It was discovered that the resulting sensor responded to hydrogen peroxide in an acidic solution containing certain concentrations of potassium iodide. A linear response over a range of 1.6 × 10-7 mol·L-1 to 9.6 × 10-5 mol·L-1 was recorded and the interference caused by the inorganic ions was very limited. Later, Li and Wang used cellulose acetate as the carrier for Rh 6G to detect the nitrites through a similar fabrication technique [85].

mPOFs were also used to fabricate gas sensors with a considerable increase in sensitivities compared to conventional FOSs. Wang et al. reported a carbon dioxide gas sensor composed of 547 hollow channels which were coated with porous ethyl cellulose layers doped with phenol red [86]. In order to achieve reversible measurements, cetyltrimethyl ammonium hydroxide (CTAOH) was added into the film as the phase-transfer agent. The resulting sensing film contains an ion pair of quaternary ammonium and deprotonated phenol red, which allows for a reversible reaction between phenol red and carbon dioxide [87]. The sensor showed a linear response towards carbon dioxide mixed in nitrogen over a range of 0-20 v/v% and the detection limit was determined to be 0.5 v/v%. The sensor reproducibility was found to be stable over 8 cycles of repeated measurements and only acidic gases were found to produce major interference. Later, Yang employed a sol-gel technique for the fabrication of a mPOF oxygen sensor with ruthenium (II) chloride as the indicator [88]. The ruthenium compound was coated on the exterior surface of a conventional PMMA fiber for the detection of oxygen [49]. The fabricated sensor exhibited a linear response to oxygen from 0-100 v/v% with a 50 ms response time. By replacing the ruthenium compound with eosin, Peng et al. developed an ammonia gas sensor using a similar fabrication technique [89]. The sensors’ response range can be tailored through a hexadecyl trimethyl ammonium bromide (CTAB) co-entrapment process and the limit of detection was found to be as low as 50 ppm.

Localized surface plasmon resonance based sensors

The sensitivity of intrinsic-transmission fiber optic sensors is largely dependent on the intensity of the evanescent wave (EW). Even though the EW intensity can be enhanced by varying the geometry of the fibers, the interaction between the EW and trace analyte amounts is frequently too weak to obtain reliable sensing results. To resolve this problem, a novel detection scheme-localized surface plasmon resonance (LSPR) has been adopted to improve the intrinsic-transmission systems, especially in the field of biological analyte sensing.

A full description of the LSPR effect has been explained in literature [90-92], hence only a compact version of the relevant theories will be discussed herein. Prior to elucidating the theories of LSPR, it is important to distinguish LSPR from surface plasmon resonance (SPR). SPR and LSPR effects can both be attributed to the photo-driven coherent oscillations of free electrons on the surface of a metal substrate surrounded by a dielectric medium. The fundamental difference between SPR and LSPR is the location of the electrons. SPR happens on a thin metal film while LSPR occurs on the surface of a nanoparticle. Compared to SPR, LSPR is highly sensitive to the local dielectric environment variations within a much shorter range from the metal surface (40-50 times less than SPR), which makes it an ideal candidate for the detection of ultra-low concentrations of bio-analytes [93,94].

Theoretical explanations for the LSPR effect were provided by Gustav Mie who derived analytical solutions from the Maxwell’s equation [95]. According to Mie, a perfect spherical nanoparticle was assumed to be surrounded by a homogeneous medium which can be described by bulk optical dielectric functions, hence the light extinction properties (σ ext) of the nanoparticles can be attributed to absorption (σ abs) and scattering (σsca ) . If the particle size is significantly smaller than the wavelength of the incident light (r/λ < 0.1), then absorption dominates the equation (Equation. 4) [44].

Equation (4)

Where, εm is the dielectric constant of the surrounding medium, εr and εi represent the real and imaginary components of the particles’ dielectric functions, respectively. N is the electron density of the particle and r is the particle radius. χ reflects the shape of the particle, it equals 2 in the case of a sphere and larger values will be assigned if the particle has higher aspect ratios [96]. Here, εr can be further expressed in the following equation [44]:

Equation (5)

Where, ωp and γ present the plasmon frequency and damping parameter of the particle, respectively. If εr is close to -2εm (the resonance conditions), the dominator in Equation 4 would be minimized and the electromagnetic (EM) field is enhanced compared to the incident field. Equation 5 can be simplified if the resonance frequency occurs in the visible and near-infrared regions ( ωp >> γ ) [44]:

Equation (6)

By substitutingEquation, Equation, Equation into Equation 6, we can obtain [44]:

Equation (7)

Where, λmax is the maximum absorption frequency of the LSPR band immersed in the medium which has the refractive index of nm , and λp corresponds to the plasmon wavelength of the particle. According to Equation 7, the relationship between a LSPR absorption peak and the refractive index of the surrounding medium can be approximated to be linear over a small range of indices. The sensitivity (S) of a LSPR sensor based on the shift of the plasmon peaks (nm) with respect to the change of the medium refractive index can be defined as:

Equation [nm·RIU-1] (8)

For a LSPR POF biosensor, the sensitivity can also be defined as:

Equation [nm·L ·mol-1] (9)

Where, c stands for the concentration of the biological analytes.

Under the aforementioned resonance conditions, Equation 4 can be further simplified to become:

Equation (10)

It is clear that the extinction coefficient of the particle also responds to variations in the refractive index of the surrounding medium due to the term (Equation in the Equation 10.

Both LSPR peak shift and absorption variations with respect to the medium’s refractive index have been employed for the fabrication of LSPR POF sensors. However, due to the intrinsically higher accuracy of the wavelength determination by modern instrumentation and the minimal interference caused by extraneous optical power fluctuations, LSPR peak shift based detection mechanisms have become more prevalent in recent advancements of LSPR optical sensors [44,93,97].

Compared to the booming applications of LSPR GOF sensors in recent years, the development of LSPR POF sensors is severely hindered, which mainly resulted from the difficulty of employing sol-gel techniques onto POF surface. Among the handful of LSPR POF sensors reported, the majority of them are based on the same configurations of LSPR GOF sensors with little improvements.Chen et al. developed a LSPR POF sensor to detect the concentration of hydrofluoric acid (HF) [98]. A thin layer of silicon dioxide bearing amine moieties was first attached onto the surface of a PMMA POF using a typical sol-gel technique. Then AuNPs were immobilized onto the silicon layer via electrostatic adsorption. The attached AuNPs layer was subsequently covered with a layer of silicon oxide matrix that originated from tetramethoxysilane (TMOS) as the sensitive coating. The HF detection mechanism is based on the intensity variations of the output light signals when the sensitive coating on AuNPs is etched by HF. Although, the author’s initial incentive of using PMMA POF was to avoid the decomposition of fibers by HF that would occur for the GOFs, the use of a silicon layer for the attachment of AuNPs still resulted in the destruction of the sensor after prolong exposure.

Recently, a LSPR POF sensor was reported by Cennamo et al. for the detection of TNT using molecularly imprinted polymers (MIP) as the sensing layer [99]. Five-branched gold nanostars (AuNSs) were first dispersed in a pre-polymeric mixture that contained TNT as the template molecule. Then, the mixture was dropped onto a side polished PMMA POF where the polymerization was carried out at elevated temperatures. The template molecules were subsequently extracted by washing with ethanol, leaving specific binding sites for TNT. AuNSs have much better sensitivity than AuNPs due to their high aspect ratios, this translated into high sensitivity for the reported sensor. The sensor sensitivity was determined to be 8.3 × 105 nm·moL-1 for a tapered POF, which is thirty times more sensitive compared to the TNT sensors reported previously [99].

Jin et al. incorporated thiol and amine functionalities onto the surface of PMMA POFs through direct surface chemical modifications, allowing for subsequent covalent bonding or electrostatic adsorption of colloidal AuNPs [100]. It was discovered that the sensitivity of the LSPR POF sensor was substantially affected by the chemistries employed for the AuNP immobilization. AuNPs immobilized on both thiolated PMMA POFs showed higher sensitivities compared to aminated PMMA POFs. Afterwards, Jin et al. functionalized surface immobilized AuNPs with glycopolymer brushes carrying glucose moieties for the detection of concanavalin A (Con A) [101]. The “glycocluster effect” induced by pendent carbohydrate moieties enabled a stronger affinity for Con A binding, which resulted in a dramatic expansion of the sensors’ response range. It was reported that, the limit of detection of the LSPR sensor was 1.3 nmol·L-1 with a saturated response at 1054.2 nmol·L-1

Similar to LSPR POF sensors, POFs have been successfully employed in the fabrication of surface plasmon resonance (SPR) optical sensors. The conventional SPR optical sensors are based on Otto configuration [102] and later improved Kretschmann configuration [103]. However, these prism based configurations suffer complex mechanical and optical structure, bulky size and difficult to miniaturize [104,105]. These problems have driven researcher to use optical fibers as the host for SPR since both prism and optical fiber can generate EW at surface due to TIF. Some experimental and theoretical work have been reported recent years on SPR sensors (mostly based on GOFs), showing a great potential of this new generation fiber optic SPR sensors [104-108].

Cennamo et al. adapted classic fabrication technique of SPR GOF sensors in development SPR POF sensors [109]. In the first configuration, a layer of gold film, 40 nm thick, was sputtered coated onto cladding stripped PMMA POF. In the second configuration, microposit S1813 photoresist was dip coated onto the fiber before gold sputter coating. The experimental test results showed, with the photoresist buffer layer, the proposed sensor has a greater linear response range from 1.332 to 1.418. While, the response range for the sensor without buffer layer was considerably lower due to light dissipation. The resolution and signal to noise ratio (SNR) were found also higher for the sensor with the buffer layer. In the refractive index medium of 1.354, resolution was found to be 0.00059 RIU and sensitivity was determined to be 2533 nm·RIU-1. With the successful fabrication of POF based SPR sensor, Cennamo later demonstrated the great potential of this sensor in the field of detecting biomolecules and aqueous chemicals [110]. By immobilisation of transglutaminase (tTG) on the gold layer, the SPR POF sensor was able to detect antitransglutaminase (anti-tTG) in the range of 30 nM and 3000 nM. On the other hand, by coating a layer of molecular imprinted polymer (MIP) on the gold layer, the proposed SPR POF sensor has the capable of specific monitoring of trinitrotoluene (TNT) and L-nicotine [111,112].

Besides using SI polymer fibers, SPR also has been incorporated into PCF or mPOF. Theoretical evaluation the performance of SPR PCF sensor was reported by Lu et al. [113]. By using finite element method (FEM), a large-mode-area PCF with a thin layer of silver coated outside shows the size and number of air holes have limited effect on the sensitivity, while both spectral and intensity resolution were found in the range of 8.3 × 10-5 and 9.4 × 10-5 RIU. About the same time, Wang et al. reported a SPR sensor based on a side-hole mPOF [114- 122]. Unlike previous techniques that deposited metals from the fluid onto the inner surface of holes, they sputter coated a gold layer onto the core of slotted fiber. Two SPR frequencies were observed at 560 nm and 620 nm when the sensor was tested in the fluids of refractive indices of 1.38 and 1.41, respectively. The sensitivity was estimated to be 2000 nm·RIU-1 [120-122].


This paper has presented a brief review of the recent progress of POF sensors. The main thrust of employing POFs originated from their high flexibility, high tensile strain, good gas and liquid permeability and in particular, versatile surface functionalization pathways. A wide range of sensing technologies has been successfully implemented in the fabrication of POFs FOSs, such as monolayer graphene, FBG, LSPR/SPR and acoustic/ultrasound. However, it is also noted that some POF sensors fabrication methods (e.g. sol-gel techniques) were directly transferred from GOF sensors without utilizing POFs’ unique properties, which resulted in similar or worsen sensing performance. Therefore, further work is still required to fully explore POFs potential in the field of FOSs.


The authors would like to acknowledge the University of New South Wales (UNSW), Faculty of Engineering Early Career Researcher Faculty Research Grant (ECR/FRG) for funding of this research.


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