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Photonics 2019, 6(2), 36;

Latest Achievements in Polymer Optical Fiber Gratings: Fabrication and Applications
ITEAM Research Institute, Universitat Politècnica de València, Camino de Vera, s/n 46022 Valencia, Spain
I3N& Physics Department, Universidade de Aveiro, Campus Universitário de Santiago, 3810-193 Aveiro, Portugal
Author to whom correspondence should be addressed.
Received: 18 February 2019 / Accepted: 26 March 2019 / Published: 29 March 2019


Grating devices in polymer optical fibers (POFs) have attracted huge interest for many potential applications in recent years. This paper presents the state of the art regarding the fabrication of different types of POF gratings, such as uniform, phase-shifted, tilted, chirped, and long period gratings, and explores potential application scenarios, such as biosensing and optical communications.
polymer optical fibers; gratings devices; optical filters; fiber sensing

1. Introduction

Polymer optical fibers (POFs) show attractive characteristics when compared with silica fibers, such as low Young’s modulus, high failure strain, high flexibility, and bio-compatibility [1]. Different kinds of plastic material with unique advantages can be used for POF fabrication besides polymethyl methacrylate (PMMA), which is the most common material with a low cost [2]. Examples of these materials are low water absorption cyclic olefin copolymers (TOPAS) [3], high glass transition temperature cyclic-olefin polymer (ZEONEX) [4], excellent clarity and impact strength engineering plastic (Polycarbonate) [5], biodegradable and biocompatible poly(D,L-lactic acid) (PDLLA) [6], and low-loss cyclic transparent amorphous fluoropolymers (CYTOP) [7]. In addition to fiber materials, several types of POFs are available in the current market with different core sizes and structures, such as small-diameter step-index (SI) POF, small-diameter microstructure POF, commercial grade-index (GI) POF, and commercial large-diameter PMMA POF, as shown in Table 1. Extended reviews about the potential applications of these fibers can be found in the literature as follows. Koike et al. [8] reviewed the status of POFs and achievements on GI POF as a promising candidate for the next generation of optical fibers. Zubia et al. [9] reviewed the most significant features of POFs, including the main types, manufacturing, and potential applications in 2001. Polishuk [10] gave a view about potential large-core POF for low-bit-rate and short distance applications. Micro-structured polymer optical fibers (mPOF) were inspired by photonic crystal fibers, first invented by Knight et al. [11] in 1996; Argyros et al. [12] proposed new potential applications for these POF structures, and also showed their easier single-mode performance compared with step-index POFs, due to the fabrication process.
Due to increasing numbers of emerging services, such as intelligent home systems, visible light communications, etc., in indoor networks, the increase of high-capacity demand shifts from long-haul systems to short-range communication links. Indeed, POFs are good candidates for short-range communications [13,14,15,16,17,18,19,20,21], with low weight and high transmission capacity. Accordingly, Professor Koike and his research group demonstrated data transmission over POF in 1995 [22], where they reported 2.5 Gb/s 100 m data transmission using GI POF at 650 nm wavelength; more recently, in 2016, they developed 120 Gb/s GI POF, as well as the ballpoint pen interconnection technology for uncompressed 4K/8K video transmission [23]. Recent achievements in POF-based transmission networks have led to promising applications in future home networks, such as Pinzon et al. [24], where a five-channel visible wavelength-division multiplexing (WDM) system was transmitted over 50-m step index POF links with a 2 Gb/s, bidirectional, real-time link. Moreover, Osahon et al. [25] has demonstrated gigabit-per-second transmission over a short-range step-index POF using a multilevel pulse amplitude modulation (PAM-M) scheme, based on a laser diode (LD) as the optical source, which also shows successful simultaneous transmission of 16-QAM 40 MHz bandwidth wireless local area network (WLAN) and 64 quadrature amplitude modulation (QAM) long term evolution (LTE-A) bands. Among recent achievements, Forni et al. [26] must be highlighted, due to their simultaneous transmission of an IEEE 02.11n 16-QAM 40 MHz bandwidth WLAN, 964 QAM LTE-A bands, and 1.7 Gb/s 4-PAM baseband signals over 50 m of 1-mm core diameter GI POF for in-home networks.
Sensing is also an emerging area of POF applications under research, as stated in the extensive literature. Peters et al. [27] presented a review work focused on strain and temperature sensing applications, based on POFs using different solutions. POF-based sensing techniques can be classified on intensity modulation sensing, Brillouin scattering, and wavelength sensitivity grating devices. Bilro et al. [28] presented a review paper about intensity modulation sensing, where all sensors include a light source, an optical fiber, and an optical spectrum analyzer or a photodetector when the accuracy is not so critical, such as structural health monitoring [27,29], deformation monitoring [30], medical instrument [31,32,33,34], environment monitoring [35,36], mechanical measurement [37,38,39], and chemical detection [40,41]. The second technique, based on Brillouin scattering in POFs [26], is mainly focused towards distributed sensing, such as structural health monitoring by POF strain sensor technology [42], according to the fundamental properties of Brillouin scattering in POF as reviewed by Mizuno et al. [43].
The last technique, based on wavelength sensitivity grating devices, is the most promising area for POF sensing. In contrast with the applications of grating devices in silica fiber, which have been under intense research for more than 30 years [44], the first POF Bragg grating (POFBG) was demonstrated by Peng’s group in 1999 [45]. Since then, the literature has presented a large number of papers reporting significant achievements, such as Dobb et al.’s [46] report in 2005 on the first FBG in few mode and endlessly single mode mPOFs, using a continuous wave laser at 325 nm wavelength; the first ultraviolet (UV) inscription of Long Period Grating in POFs published by Saez et al. [47] in 2010; or the first FBG in multimode POF at 827 nm wavelength, published by Johnson et al. [48] in 2010.
The main drawback of PMMA fibers is water absorption, which can be reduced by using other polymer materials. An example is TOPAS, a cyclic olefin copolymer with moisture absorption that is at least 30 times lower than that of PMMA. In this sense, Wu et al. reported the first experimental results about a humidity-insensitive POF Fiber Bragg Grating [49]. Moreover, Woyessa et al. [4] demonstrated the very first low, endlessly single-mode and humidity-insensitive mPOF made of ZEONEX-grade 480R with a glass transition temperature of 138 °C, and the first FBG was inscribed in ZEONEX mPOF at a low-attenuation 850 nm region. Polycarbonate is another material, first introduced by Fujitsu in 1989 [50], which exhibits excellent transparency and impact strength. Fasano et al. [5] reported the first experimental demonstration of an endlessly single-mode polycarbonate mPOF, and also inscribed the first FBG in polycarbonate mPOF. Last but not least, cyclic transparent fluoropolymers (CYTOP) exhibit excellent transmission characteristics from the visible to near-infrared spectrum, due to the optical absorption wavelength shift to 7.7~10 μm, which exceeds the transmission limit of other polymer materials, such as high-loss PMMA, induced by the high overtone vibration of C–H at 3~3.5 μm. This, therefore, allows Bragg gratings to be inscribed in CYTOP fibers by using a femto-second laser [51,52,53,54,55,56] and phase mask method [57,58,59].
As happens in silica fibers, special grating devices are attractive for a variety of applications. Birefringent gratings have been employed to change the polarization state of light at different wavelengths [60,61], and laser micromachining has been used for obtaining POF gratings with different microstructures in the cladding, in order to enhance their humidity response time [62] with a high strain sensitivity [63]. A Fabry–Perot cavity based on POF gratings was fabricated by Dobb et al. [64], phase-shifted (PS) FBGs in POF were obtained by uniform UV exposure of the central part of 1-cm-long gratings [64], and tilted FBGs were reported by Hu et al. in 2014 [65] in step-index POFs, among others included in [66]. Finally, chirped FBGs were fabricated by using a chirped phase mask in 2017 [67].
Previous literature includes extensive reviews published by Webb [1], Luo et al. [66], Canning [68], Marques et al. [69,70], Broadway et al. [71], Berghmans et al. [72], and Nogueira et al. [73], focusing on the uniform POF gratings fabrication and applications. Due to the emerging POF applications in communications and sensing, intense work has been done in recent years towards obtaining a short, flexible, and reliable fabrication process for gratings in these fibers.
After discussing historical records and motivation in the introduction section of this paper, we report below a review work about the latest results on POF grating device fabrication and applications, structured as follows. Recent results on POF gratings fabrication using different UV lasers and fibers will be reported in Section 2, and Section 3 will focus on recently identified potential applications of different POF grating devices. Finally, Section 4 summarizes the main conclusions and outlines the most promising POF gratings research lines, to be followed within the short- and mid-term.

2. Fabrication of Polymer Optical Fiber Gratings

POF Bragg gratings (POFBGs) are typically fabricated by direct writing [74], Sagnac interferometry [75], and phase mask [1] techniques, although the preferred POFBG fabrication technique is the latter one, due to easy implementation in spite of the limited flexibility. Direct writing provides flexibility in terms of structure and wavelength, but the femtosecond laser system is required for FBG irradiation, and the resolution imposes limitations on the achievable low wavelengths. Long period gratings are usually obtained by direct writing [75,76], heat imprinting, and amplitude masks [77,78].
In this section, we present the recent achievements in the optimization of the fabrication process, as well as gratings inscription in different types of doped and undoped POFs, and illustrate the flexibility of the fabrication procedures.

2.1. Optimization of the Fabrication Process

Gratings are fabricated in fibers, due to the photosensitivity of polymer material under UV, which leads to the fiber refractive index change after UV absorption. Indeed, photosensitivity strongly depends on the wavelength and the inscription mechanism, as was completely detailed by Luo et al. [66]. Since the Bell laboratories discovered this around 1970s [79], the absorption of 325 nm wavelength UV radiation was identified as the preferred technique for refractive index change in PMMA material. Depending on the power and wavelength of the absorbed light, several mechanisms occur in combined reactions, such as photo polymerization, photo degradation, and cross-linking change between the polymer chains. Yu et al. [80] reported refractive index modification by photo-isomerization, and also showed that polymer fiber cores doped with dopants (i.e. trans-4-stilbenemethanol, or TS) exhibit different refractive index changes under UV radiation. Saez et al. [81] reported that the photosensitivity of undoped PMMA mPOF can be increased by straining the fiber during photo inscription, which is evidence of photodegradation and paved the way for undoped PMMA POF grating irradiation under 325 nm wavelength.
The stability of POF gratings is a critical issue mentioned by several papers [67,82,83,84,85]. Pre-annealed POFs allow the fabrication of more stable short-term performance gratings at both greater strain and higher temperatures [85]. However, both non-annealed and annealed TS-doped polymer optical fibers were studied in terms of FBG stability, and the post-inscription thermal annealing process was necessary to produce stable gratings [83]. POF grating fabrication has been reported using different lasers, such as an 800 nm Ti:sapphire fs laser system [74,86], a 532 nm Nd:YVO4 laser system [77,87], a 387 nm Ti:sapphire fs laser system [88], a 355 nm Nd:YAG laser [89], a 325 nm optical parametric oscillator (OPO) pulsed laser, a dye laser, an He–Cd laser [81,90,91,92,93,94,95], and a 248 nm KrF excimer laser system [73,96]. Although 325 nm was the first irradiation wavelength reported by Peng’s group [45], and initially 248 nm wavelength was not considered suitable for polymer fiber Bragg grating writing, due to high absorption, the first successful Bragg grating inscription in 30 seconds using low flow and a repetition rate at 248 nm UV light opened a new field of interest for grating irradiation [96]. Since then, the research work on gratings inscription using 248 nm wavelength has been continuously growing. A typical POF FBG irradiation system is shown in Figure 1, where the pulse power and repetition rate can be optimized [97,98] in order to shorten the fabrication time, as will be shown below.

2.2. Different Polymer Materials

Due to the low photosensitivity of pure PMMA fiber [93], doped POFs have attracted researchers’ interest [80,98,99]. Peng’s group employed a step-index, multimode PMMA fiber with an organic dye doped core [100] for grating irradiation under a 325 nm UV beam, and obtained seven peaks in the reflected spectrum. The same group fabricated another fiber with low-concentration ethyl and a benzyl methacrylate doped core, which led to obtaining a −28 dB transmission FBG with 85 min exposure [90]. Tam’s group investigated a step-index PMMA POF with a TS (1% w.t.) and diphenyl sulfide (DPS) (5% mole) doped core (diameter of 8.2 µm), as well as pure PMMA cladding (diameter of 150 µm). Both dopants were used to increase the refractive index and enhance photosensitivity [80], and they obtained one FBG of about −10 dB transmission after 10 min. Saez et al. [93] reported a highly photosensitive mPOF using Benzyl dimethyl ketal (BDK )as a dopant in the core, and −23 dB transmission was achieved after 13 min, since the lack of extra dopants required to compensate for the index reduction allows for shorter times compared with BDK-doped step-index fiber [99]. Recently, Hu et al. [101] improved the fiber drawing technology with selected center-hole BDK doping in mPOF, for a rapidly growing process with 83% reflectivity in 40 s. Tam’s group investigated a new dopant material, diphenyl disulphide, which enables a fast and positive refractive index change with a low ultraviolet dose, and leads to Bragg gratings fabrication after just 7 ms under 325 nm-wavelength UV signal irradiation [102].
Pospori et al. [84] and Pereira et al. [103] fabricated FBGs in BDK-doped POF using 248 nm and 266 nm wavelength irradiation, respectively, and obtained strong POFBGs with a single short laser pulse (15 and 8 ns of duration), as shown in Figure 2, which is even compatible with the fiber drawing process. Bragg gratings inscription in the 850 nm spectral region was also reported by using step-index PMMA POF irradiation, using a 248 nm krypton fluoride (KrF) excimer laser system, which only took 0.4 seconds with 100 Hz pulse repetition, as shown in Figure 3. In this fiber, the cladding material is pure PMMA, while the core is PMMA doped with TS (1% w.t.) and diphenyl sulfide (DPS) (5% mole) to enhance the photosensitivity and increase the refractive index [98].
Marques et al. [104] reported the inscription of gratings in POFs made of different materials (TOPAS, ZEONEX, and Polycarbonate) under 248 nm wavelength, and compared it with the same fiber irradiation under 325 nm, resulting in a reduction of the irradiation time by at least 16 times (Table 2) and better stability when 248 nm wavelength is employed.
Min et al. [58] obtained the first 600 nm wavelength grating with commercial CYTOP POF, using a 248 nm KrF laser system with a repetition of 40 Hz and average pulse energy of ~0.60 mJ during ~60 min, as shown in Figure 4, with potential applications in the visible range.

2.3. Special Grating Devices

Recently, a novel bandpass transmission filter based on PS FBG at telecom wavelength [105] was obtained using the Moiré method by 325 nm Kimmon laser system exposure for about 20 mins, as shown in Figure 5. A Moiré structure is formed by superimposing two gratings of equal amplitude but with slightly different periods. Figure 6a shows the result of two superimposed pulses on a single-mode, BDK-doped mPOF by using a 248 nm KrF laser emitting an output pulse power of 2.5 mJ energy and a 15 ns duration [106]. The obtained grating showed 0.035 nm bandwidth and 8 dB in the rejection band, with a high level of flexibility and no need for strain accuracy. At the 850 nm wavelength region, PS FBG was also obtained directly during the grating fabrication, by placing a narrow blocking aperture in the center of the UV beam (see Figure 6b) [107]. A high-quality Bragg grating structure was obtained with −16.3 dB and −13.2 dB dips in transmission. The only drawback is one narrow line needing blocking accuracy, which must be put on the phase mask.
Although chirped FBGs in POF were proposed for dispersion tuning without a wavelength shift in 2005 [108], the first chirped FBG in POF was inscribed in 2017 using an KrF excimer laser, operating at 248 nm, and a 25-mm long chirped phase mask, customized for 1550-nm grating inscription [67]. The laser pulse rate was 1 Hz (5 mJ), and only a few shots were employed for the grating response depicted in Figure 7a, with a 3.9 nm bandwidth and 1.2 nm/cm chirp. The chirped phase mask method offers significant stability, with high cost and no flexibility as its main drawbacks. Since then, different techniques have been demonstrated to be valid for fabricating chirped gratings in POF. Theodosiou et al. used the femtosecond direct writing method to obtain chirped FBG in commercial CYTOP POF [52], which consisted of 2000 periods, with a total length of ~4.5 mm and a 10-nm bandwidth (chirp of ~2.22 nm/mm), as shown in Figure 7b. A femtosecond laser direct writing was used for flexible chirped grating writing, with limitations for low wavelengths. However, the first tunable chirped FBG was fabricated in a tapered, BDK-doped mPOF by using a uniform phase mask under 248 nm UV [109]. The spectral reflected power of a 10 mm grating with chirp of ~0.26 nm/mm under 1.6% strain is shown in Figure 7c, and the tunable properties were given by the strain and temperature sensitivity, with 0.71 ± 0.02 pm/µε and 56.7 pm/°C [109,110], as shown in Figure 8. However, largely chirped POFBGs have been also fabricated by hot water-assisted gradient thermal annealing, as shown in Figure 7d [111], where one grating with ~1.1 nm/mm chirp was obtained. The simplicity of this method is one of its main advantages, since no special phase mask or additional etching are needed, and it enables easy control tuning of the central wavelength and chirp characteristics.
Finally, regarding long period gratings in POF, the extensive literature during the last years shows different mechanisms and methods to be used for fabricating them in POF [47,75,76,87,95,112]. Recently, Min et al. [113] demonstrated a −20 dB transmission LPG in mPOF (see Figure 9a) using the point-by-point method, with an slit width of 0.2 mm; the beam was shifted 1 mm for inscribing every point, and 25 steps were completed to obtain an LPG total length of 25 mm. Each inscription point was irradiated by two 15 ns pulses emitted by the UV laser at 1 Hz frequency repetition rate, and therefore, a 2 s irradiation time means a significant reduction from the 42 s per point writing time reported in a previous work [95]. The strain sensitivity about −2.3 ± 0.05 nm/mstrain was measured for increasing strain, whereas −2.25 ± 0.05 nm/mstrain was measured for decreasing strain, due to polymer hysteresis, as shown in Figure 9b; this is slightly larger than the value presented in the previous literature, which ranged from −1.40 to −1.44 nm/mstrain for increasing strain and between −1.30 and −1.40 nm/mstrain for decreasing strain [114].

3. Applications

Dispersion compensation using chirped POFBG was first proposed in 2005 [107], but the experimental demonstration of a largely tunable dispersive device based on a chirped FBG in mPOF was published by Min et al. [115]. Figure 10 depicts the reflected spectral power with a bandwidth from 0.11 to 4.86 nm, as well as the group delay variation under strain, which corresponds to a tunable dispersion from 513.6 to 11.15 ps/nm, respectively, with potential applications in both optical communications and microwave photonics systems.
Among the POF applications, due to polymer characteristics mentioned in the Introduction section of this paper, strain sensing is the most popular application. However, strain sensing under variable temperature and humidity conditions is always an issue for POF sensing. Min et al. [116] demonstrated that the effective bandwidth of the tunable chirped POFBG is highly dependent on the strain, and remains practically constant with temperature and humidity changes, which can be used in combination with wavelength measurement, as shown in Figure 11, to develop strain sensors under temperature- and humidity-variable environments. The strain sensitivity is 9.02 ± 0.02 pm/µε, which is higher than previous results [109] due to larger etching [92].
One of the recent challenges for fiber optic temperature sensing is found in biomedical applications. An essential feature of these systems is the possibility of detecting temperature spatial distributions, also known as thermal maps [117]. A linearly chirped POFBG has been demonstrated as a semi-distributed temperature sensor capable of monitoring the temperature profile along the grating length for minimally invasive scenarios [118]. As shown in Figure 12, the chirped POFBG has been placed close to a radiofrequency applicator, with a tip inserted in situ of the target—the applicator connected to the Radio Frequency generator. The reflection spectrum was detected by Optical Backscatter Reflectometer (LUNA OBR 4600), and the temperature gradient was estimated with the Gaussian model. High sensitivity of chirped POFBG supports the detection of spatially non-uniform temperature by means of spectral reconstruction, which indicates that chirped FBG in mPOF can provide significant advantages for thermal detecting in bio-medical applications.
Furthermore, chirped POFBGs fabricated with chirped phase mask have been also demonstrated to provide accurate distributed pressure sensing [67]. The grating was subjected to pressure at various spatial position points of the grating, as shown in Figure 13, and the reflected spectral power showed a wavelength dip related to the pressed region, which can be used for different sensing applications.
Another interesting application is provided by health equipment for the dynamic monitoring of gait. An array of five FBGs inscribed in CYTOP fiber [119] was embedded in a cork insole, as shown in Figure 14. The advantages of POF (e.g., higher flexibility and robustness) enabled monitoring patients with higher body mass compared with similar systems based on silica fiber, with a mean sensitivity of ~8.14 PM/kPa, which is almost four times higher than silica FBGs (~2.51 pm/kPa).
Surface plasmon resonance (SPR) is an accurate and reliable technique for determining the change of density at the interface between a dielectric medium and a metal, which has attracted huge attention for biochemical sensing in microfluidic systems. Hu et al. [120] reported the first excitation of SPR at near-infrared telecom wavelength with gold-coated POF tilted FBGs. They show the transmission dips corresponding to the orthogonally polarized modes, coupled in a 50-nm gold-coated 6° tilted FBG immersed in a solution of refractive index 1.408. The transmission spectrum when the grating is immersed in different calibrated liquids covering a large SRI (sounding refractive index) range of 2.5 × 10−2 RIU (refractive index unit). The refractometric sensitivity was measured up to ~550 nm/RIU, with a wavelength shift as a function of the SRI value, which is suitable for in situ operation.
Finally, piezoelectric transducers of ultrasounds are widely used in the biomedical area, but the main drawback is their sensitivity to electromagnetic fields. Optical fibers are promising for replacing piezo electric transducers, with the benefit of electromagnetic interference immunity and with good sensor sensitivity and size for ultrasonic detection. POF shows better robustness and sensitivity to pressure than silica fiber, as required by ultrasound detectors. Broadway et al. [121] presented the first ultrasonic detection at 5, 10, and 15 MHz by using a tilted FBG in commercial CYTOP fibers, as shown in Figure 15, which paves the way towards its eventual applications.

4. Conclusion and Outlook

Significant progress has been obtained during recent years in POF grating devices fabrication and applications, in order to allow fast fabrication of POF grating devices under 248 nm and 266 nm wavelength UV, such as one short UV pulse (15 ns) for chirped POFBG fabrication. Besides the benefit of potential grating fabrication in the drawing tower, special grating structures also take advantage of the short irradiation time to reduce the stability requirements in the fabrication setup.
Besides humidity-, temperature-, and strain-sensitive devices as the main applications of uniform POF FBG, special grating devices open new perspectives. As the main relevant examples, this paper reviews chirped POFBGs for high-resolution thermal detection in the biomedical area, which show higher sensitivity and bio-compatibility than silica ones. In addition, tilted POF FBG for SPR sensing and tilted FBGs for high-resolution acoustic detection are promising for in situ operation. Furthermore, optical communication applications, such as dispersion compensation and slicing broadband sources for WDM systems, among others, will benefit from the POF advantages in the implementation of future indoor networks.
To conclude, POF gratings show attractive performance from the sensing area to the short-range optical communication area. However, as we know, most of the POFs for grating devices fabrication are homemade, which still need more time to make this technology mature for potential real applications; from this perspective, grating devices in commercial CYTOP POF are promising for real applications. More progress is required to achieve strong and stable devices in reduced-loss and low-price POFs.

Author Contributions

Writing—original draft preparation, R.M., B.O., and C.M.; writing—review and editing, B.O. and C.M.


This research was funded by Research Excellence Award Programme GVA PROMETEO 2017/103 and Fundação para a Ciência e a Tecnologia, I.P. (FCT) through the program UID/CTM/50025/2019, by the National Funds through the Fundação para a Ciência e a Tecnologia / Ministério da Educação e Ciência, and by the European Regional Development Fund under the PT2020 Partnership Agreement. This work is also funded by national funds (OE), through FCT, in the scope of the framework contract foreseen in the numbers 4, 5, and 6 of the article 23, of the Decree-Law 57/2016, of August 29, changed by Law 57/2017, of July 19, the Science Foundation of Heilongjiang Province of China (F2018026) and University Nursing Program for Young Scholars with Creative Talents in Heilongjiang Province (NPYSCT-2018012).


The authors acknowledge the supported by FCT, Research Excellence Award Programme GVA PROMETEO 2017/103, and the Science Foundation of Heilongjiang Province of China.

Conflicts of Interest

The authors declare no conflict of interest.


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Figure 1. Typical POF FBG irradiation system; image adapted from [58].
Figure 1. Typical POF FBG irradiation system; image adapted from [58].
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Figure 2. Transmission and reflection spectrum of Fiber Bragg Grating in BDK-doped micro-structured polymer optical fiber (mPOF) with one single 266 nm wavelength pulse; image adapted from [103].
Figure 2. Transmission and reflection spectrum of Fiber Bragg Grating in BDK-doped micro-structured polymer optical fiber (mPOF) with one single 266 nm wavelength pulse; image adapted from [103].
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Figure 3. Reflected spectrum of a FBG in a trans-4-stilbenemethanol (TS)-doped, step-index POF, inscribed using a 100 Hz repetition rate and pulse energy of 0.50 ± 0.02 mJ in 0.4 seconds (40 pulses); image adapted from [98].
Figure 3. Reflected spectrum of a FBG in a trans-4-stilbenemethanol (TS)-doped, step-index POF, inscribed using a 100 Hz repetition rate and pulse energy of 0.50 ± 0.02 mJ in 0.4 seconds (40 pulses); image adapted from [98].
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Figure 4. Reflected spectrum of the FBG in cyclic transparent amorphous fluoropolymers (CYTOP) fiber; image adapted from [58].
Figure 4. Reflected spectrum of the FBG in cyclic transparent amorphous fluoropolymers (CYTOP) fiber; image adapted from [58].
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Figure 5. Phase-shifted (PS) FBG fabricated by 325 nm irradiation: (a) uniform FBG (first fabrication step), (b) PS FBG (Moiré structure based on two overlapped uniform gratings); image adapted from [105].
Figure 5. Phase-shifted (PS) FBG fabricated by 325 nm irradiation: (a) uniform FBG (first fabrication step), (b) PS FBG (Moiré structure based on two overlapped uniform gratings); image adapted from [105].
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Figure 6. PS-FBG fabrication by 248 nm irradiation: (a) Moiré overlapping method (image adapted from [106]); (b) a narrow blocking in the center (image adapted from [107]).
Figure 6. PS-FBG fabrication by 248 nm irradiation: (a) Moiré overlapping method (image adapted from [106]); (b) a narrow blocking in the center (image adapted from [107]).
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Figure 7. The reflected spectral power of a chirped POFBG fabricated by different techniques: (a) chirped phase mask (image adapted from [67]), (b) femtosecond directly writing on CYTOP POF (image from [65]), (c) under 1.6 % strain with tapering method (image adapted from [109]), and (d) thermal annealing (image adapted from [111]).
Figure 7. The reflected spectral power of a chirped POFBG fabricated by different techniques: (a) chirped phase mask (image adapted from [67]), (b) femtosecond directly writing on CYTOP POF (image from [65]), (c) under 1.6 % strain with tapering method (image adapted from [109]), and (d) thermal annealing (image adapted from [111]).
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Figure 8. The reflected spectral power of chirped POFBGs (a) under different strain and (b) under different temperatures; image adapted from [109].
Figure 8. The reflected spectral power of chirped POFBGs (a) under different strain and (b) under different temperatures; image adapted from [109].
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Figure 9. (a) Transmission of Long Period Grating, and (b) wavelength change induced by increasing and decreasing strain; image from [113].
Figure 9. (a) Transmission of Long Period Grating, and (b) wavelength change induced by increasing and decreasing strain; image from [113].
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Figure 10. Tunable chirped FBG (a) reflected spectral power vs strain and (b) group delay vs strain; image adapted from [115].
Figure 10. Tunable chirped FBG (a) reflected spectral power vs strain and (b) group delay vs strain; image adapted from [115].
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Figure 11. (a) Reflected spectral power vs strain, (b) wavelength shift vs strain, and (c) bandwidth vs strain; image adapted from [116].
Figure 11. (a) Reflected spectral power vs strain, (b) wavelength shift vs strain, and (c) bandwidth vs strain; image adapted from [116].
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Figure 12. (a) Schematic of thermal ablation and (b) measurement of a Gaussian temperature gradient by using a chirped POFBG; image adapted from [118].
Figure 12. (a) Schematic of thermal ablation and (b) measurement of a Gaussian temperature gradient by using a chirped POFBG; image adapted from [118].
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Figure 13. (a) Setup for applying pressure and (b) measured spectrum under point pressure; image adapted from [67].
Figure 13. (a) Setup for applying pressure and (b) measured spectrum under point pressure; image adapted from [67].
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Figure 14. (a) Foot plantar area designation and sensing points and (b) FBG position in the cork insole; image from [120].
Figure 14. (a) Foot plantar area designation and sensing points and (b) FBG position in the cork insole; image from [120].
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Figure 15. Ultrasonic detection setup.
Figure 15. Ultrasonic detection setup.
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Table 1. Typical polymer optical fiber (POF) structures.
Table 1. Typical polymer optical fiber (POF) structures.
Fiber TypeTransversal SectionDiameter Main Feature
Small-diameter step-index
Photonics 06 00036 i001100~200 μmEasy coupling
Potential single-mode performance
Microstructure POF Photonics 06 00036 i002100~250 μmEasy to obtain single-mode performance
Can be made with a single material
Commercial grade-index (GI) POF Photonics 06 00036 i003490 μmLow loss
Large bandwidth
Commercial large-diameter polymethyl methacrylate (PMMA) POF Photonics 06 00036 i0041 mmLow price
Easy handling
Table 2. POFBG inscription with pulsed 248 nm KrF laser system [104].
Table 2. POFBG inscription with pulsed 248 nm KrF laser system [104].
POFsInscription Time (seconds)FWHM (nm)Reflection Band (dB)Optimal Energy (mJ)
PMMA mPOF250.4326.0
Topas 8007 mPOF250.6315.5
Topas 5013 mPOF200.6236.0
Topas step-index POF110.8315.0
Zeonex 480R mPOF150.7283.5
Polycarbonate mPOF140.6233.0

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