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Search Results (1,224)

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18 pages, 1627 KiB  
Article
Respiratory Rate Monitoring via a Fibre Bragg Grating-Embedded Respirator Mask with a Wearable Miniature Interrogator
by Nat Limweshasin, Itzel Avila Castro, Serhiy Korposh, Stephen P. Morgan, Barrie R. Hayes-Gill, Mark A. Faghy and Ricardo Correia
Sensors 2024, 24(23), 7476; https://doi.org/10.3390/s24237476 (registering DOI) - 23 Nov 2024
Viewed by 179
Abstract
A respiration rate (RR) monitoring system was created by integrating a Fibre Bragg Grating (FBG) optical fibre sensor into a respirator mask. The system exploits the sensitivity of an FBG to temperature to identify an individual’s RR by measuring airflow temperature variation near [...] Read more.
A respiration rate (RR) monitoring system was created by integrating a Fibre Bragg Grating (FBG) optical fibre sensor into a respirator mask. The system exploits the sensitivity of an FBG to temperature to identify an individual’s RR by measuring airflow temperature variation near the nostrils and mouth. To monitor the FBG response, a portable, battery-powered, wireless miniature interrogator system was developed to replace a relatively bulky benchtop interrogator used in previous studies. A healthy volunteer study was conducted to evaluate the performance of the developed system (10 healthy volunteers). Volunteers were asked to perform normal breathing whilst simultaneously wearing the system and a reference spirometer for 120 s. Individual breaths are then identified using a peak detection algorithm. The result showed that the number of breaths detected by both devices matched exactly (100%) across all volunteer trials. Full article
(This article belongs to the Section Biosensors)
11 pages, 1995 KiB  
Article
Angle-Tunable Method for Optimizing Rear Reflectance in Fabry–Perot Interferometers and Its Application in Fiber-Optic Ultrasound Sensing
by Yufei Chu, Mohammed Alshammari, Xiaoli Wang and Ming Han
Photonics 2024, 11(12), 1100; https://doi.org/10.3390/photonics11121100 - 21 Nov 2024
Viewed by 256
Abstract
With the introduction of advanced Fiber Bragg Grating (FBG) technology, Fabry–Pérot (FP) interferometers have become widely used in fiber-optic ultrasound detection. In these applications, the slope of the reflectance is a critical factor influencing detection results. Due to the intensity limitations of the [...] Read more.
With the introduction of advanced Fiber Bragg Grating (FBG) technology, Fabry–Pérot (FP) interferometers have become widely used in fiber-optic ultrasound detection. In these applications, the slope of the reflectance is a critical factor influencing detection results. Due to the intensity limitations of the laser source in fiber-optic ultrasound detection, the reflectance of the FBG is generally increased to enhance the signal-to-noise ratio (SNR). However, increasing reflectance can cause the reflectance curve to deviate from a sinusoidal shape, which in turn affects the slope of the reflectance and introduces greater errors. This paper first investigates the relationship between the transmission curve of the FP interferometer and reflectance, with a focus on the errors introduced by simplified assumptions. Further research shows that in sensors with asymmetric reflectance slopes, their transmittance curves deviate significantly from sinusoidal signals. This discrepancy highlights the importance of achieving symmetrical slopes to ensure consistent and accurate detection. To address this issue, this paper proposes an innovative method to adjust the rear-end reflectance of the FP interferometer by combining stress modulation, UV adhesive, and a high-reflectivity metal disk. Additionally, by adjusting the rear-end reflectance to ensure that the transmittance curve approximates a sinusoidal signal, the symmetry of the slope is maintained. Finally, through practical ultrasound testing, by adjusting the incident wavelength to the positions of slope extrema (or zero) at equal intervals, the expected ultrasound signals at extrema (or zero) can be detected. This method converts the problem of approximating a sinusoidal signal into a problem of the slope adjustment of the transmittance curve, making it easier and more direct to determine its impact on detection results. The proposed method not only improves the performance of fiber-optic ultrasound sensors but also reduces costs, paving the way for broader applications in medical diagnostics and structural health monitoring. Full article
(This article belongs to the Special Issue Optical Sensing Technologies, Devices and Their Data Applications)
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<p>The schematic diagram of the FP transmittance curve.</p>
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<p>Variation of error due to assumptions in FP reflectivity changes.</p>
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<p>The variation in the slope due to the FP reflectivity changes. (<b>a</b>) The reflectivity of the front and rear ends is equal; (<b>b</b>) the reflectivity of the front end is fixed at 10%, and only the reflectivity of the rear end is changed; the solid line is the reflectivity; the dotted line is the slope of the normalized reflectivity. In the legend, “S” represents the slope.</p>
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<p>The angle adjustment of end−face reflectivity based on UV Glue. (<b>a</b>) The slope of the reflectivity is asymmetric; (<b>b</b>) the slope of the reflectivity is symmetric (the green points labeled a, b, c, and d correspond to the positions where the slope is at a minimum, zero, maximum, and zero, respectively).</p>
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<p>Angle symmetry testing setup and results for the ultrasound sensor: (<b>a</b>) ultrasound detection setup (the structure diagram of the FP sensor is shown within the black dashed line), (<b>b</b>−<b>e</b>) show the ultrasound detection results when the laser wavelength is adjusted to operating points a, b, c, and d in <a href="#photonics-11-01100-f004" class="html-fig">Figure 4</a>b, respectively.</p>
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11 pages, 7949 KiB  
Article
Dynamic Excitation of Surface Plasmon Polaritons with Vector Laguerre–Gaussian Beams
by Aldo Peña-Ramírez, Tingting Zhai, Rafael Salas-Montiel and Víctor Ruiz-Cortés
Optics 2024, 5(4), 523-533; https://doi.org/10.3390/opt5040039 - 21 Nov 2024
Viewed by 271
Abstract
We investigate the dynamic excitation of surface plasmon polaritons (SPPs) using vector Laguerre–Gauss (LG) beams, which offer unique properties for manipulating the polarization and spatial distribution of light. Our study demonstrates the efficient coupling of SPPs with LG beams, characterized by their azimuthal [...] Read more.
We investigate the dynamic excitation of surface plasmon polaritons (SPPs) using vector Laguerre–Gauss (LG) beams, which offer unique properties for manipulating the polarization and spatial distribution of light. Our study demonstrates the efficient coupling of SPPs with LG beams, characterized by their azimuthal and radial indices (m,p), as well as polarization distribution type. Numerical simulations reveal that the vector nature of LG beams enables selective excitation of SPPs, depending on the polarization type of the beam. Experimental verification of our simulations is achieved using a gold circular Bragg grating and a spatial light modulator that generates vector LG beams. Leakage radiation imaging demonstrates the potential of vector LG beams for dynamic SPP excitation and manipulation. This study opens novel ways for the control of SPPs in plasmonic devices, such as modulators, and nanophotonic circuits. Full article
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<p>Dynamic excitation of surface plasmon polaritons with vector Laguerre–Gaussian beams. (<b>a</b>) Schematic of the circular plasmonic Bragg grating on gold thin film. The thickness of the grating and thin film are 20 nm and 50 nm, respectively. The grating consists of 14 concentric rings with a period of a = 0.764 μm and 0.5 duty cycle. The structure is dynamically excited with vector LG beams at normal incidence. (<b>b</b>) Optical and (<b>c</b>) scanning electron microscope images of the grating. Zoom on the grating area. (<b>d</b>) Scheme of the setup for the dynamic excitation of SPPs with vector LG beams. A spatial light modulator (SLM) is used to form the vector LG beams. Red optical path shows the path for the Fourier plane.</p>
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<p>Calculated intensity and polarization distributions of vector LG beams <span class="html-italic">p</span> = 0 and (<b>a</b>) <span class="html-italic">m</span> = 1, types I–IV, (<b>b</b>) <span class="html-italic">m</span> = 2, types I–IV, (<b>c</b>) <span class="html-italic">m</span> = 3, types I–IV, and (<b>d</b>) <span class="html-italic">m</span> = 4, types I–IV. Scale bar is 25 μm.</p>
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<p>Excitation of surface plasmon polaritons with type I–IV vector <math display="inline"><semantics> <mrow> <mi>L</mi> <msub> <mi>G</mi> <mrow> <mo>(</mo> <mn>0</mn> <mo>,</mo> <mo>[</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mn>3</mn> <mo>,</mo> <mn>4</mn> <mo>]</mo> <mo>)</mo> </mrow> </msub> </mrow> </semantics></math> beams. Distribution of the electric field and magnetic field lines for vector <math display="inline"><semantics> <mrow> <mi>L</mi> <msub> <mi>G</mi> <mrow> <mo>(</mo> <mn>0</mn> <mo>,</mo> <mi>m</mi> <mo>)</mo> </mrow> </msub> </mrow> </semantics></math> beams (<b>a</b>) <span class="html-italic">m</span> = 1, type I, (<b>b</b>) <span class="html-italic">m</span> = 1, type II, (<b>c</b>) <span class="html-italic">m</span> = 1, type III, and (<b>d</b>) <span class="html-italic">m</span> = 1, type IV, (<b>e</b>) <span class="html-italic">m</span> = 2, type I, (<b>f</b>) <span class="html-italic">m</span> = 2, type II, (<b>g</b>) <span class="html-italic">m</span> = 2, type III, and (<b>h</b>) <span class="html-italic">m</span> = 2, type IV, (<b>i</b>) <span class="html-italic">m</span> = 3, type I, (<b>j</b>) <span class="html-italic">m</span> = 3, type II, (<b>k</b>) <span class="html-italic">m</span> = 3, type III, and (<b>l</b>) <span class="html-italic">m</span> = 3, type IV, (<b>m</b>) <span class="html-italic">m</span> = 4, type I, (<b>n</b>) <span class="html-italic">m</span> = 4, type II, (<b>o</b>) <span class="html-italic">m</span> = 4, type III, and (<b>p</b>) <span class="html-italic">m</span> = 4, type IV. Scale bar is 500 nm.</p>
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<p>Experimental excitation of surface plasmon polaritons. (<b>a</b>) Optical image of the gold Bragg grating with a period of 764 nm. The two circumferences represent the inner and outer ring of the grating. Leakage radiation imaging of the excitation of SPPs with vector <math display="inline"><semantics> <msub> <mrow> <mi>LG</mi> </mrow> <mrow> <mo>(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>)</mo> </mrow> </msub> </semantics></math> (<b>b</b>) type III and (<b>c</b>) type I beams. Only type III beams excite SPPs.</p>
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<p>Experimental excitation of surface plasmon polaritons. Type I and III vector <math display="inline"><semantics> <msub> <mrow> <mi>LG</mi> </mrow> <mrow> <mo>(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>)</mo> </mrow> </msub> </semantics></math> beams. Experimental distribution of polarization of the incident field types (<b>a</b>) I and (<b>d</b>) III. Leakage radiation microscopy images of the excitation of SPPs in (<b>b</b>) the direct and (<b>c</b>) Fourier spaces for the type I and (<b>e</b>,<b>f</b>) for type III beams. Scheme of the incident fields for simulations of type (<b>g</b>) I and (<b>j</b>) III beams. Corresponding results of the excitation of SPPs in the (<b>h</b>,<b>k</b>) direct and (<b>i</b>,<b>l</b>) Fourier spaces.</p>
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<p>Excitation of SPPs with combinations of vector <math display="inline"><semantics> <msub> <mrow> <mi>LG</mi> </mrow> <mrow> <mo>(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>)</mo> </mrow> </msub> </semantics></math> type I and III beams. Scheme of distributions (<b>a</b>) D1, (<b>b</b>) D2, (<b>c</b>) D3, and (<b>d</b>) D4. The white lines represent the inner and outer grating rings. Leakage radiation images of SPPs in (<b>e</b>–<b>h</b>) the direct and (<b>i</b>–<b>l</b>) Fourier spaces for distributions D1, D2, D3, and D4, respectively. Arrows indicate the sections where leakage radiation was detected. Insets in (<b>e</b>–<b>h</b>) are magnifications in the center of the grating. Scale bar is 10 μm in (<b>a</b>–<b>h</b>).</p>
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16 pages, 7263 KiB  
Article
Inscription and Thermal Stability of Fiber Bragg Gratings in Hydrogen-Loaded Optical Fibers Using a 266 nm Pulsed Laser
by Xiangxi Zhu, Zixuan Xin, Haoming Zhu, Hongye Wang, Xin Cheng, Hwa-Yaw Tam, Hang Qu and Xuehao Hu
Photonics 2024, 11(11), 1092; https://doi.org/10.3390/photonics11111092 - 20 Nov 2024
Viewed by 411
Abstract
Fiber Bragg gratings (FBGs) have gained substantial research interest due to their exceptional sensing capabilities. Traditionally, FBG fabrication has required the use of pre-hydrogenated fibers and high-cost laser systems such as excimer lasers at 193 nm or femtosecond lasers. In this study, we [...] Read more.
Fiber Bragg gratings (FBGs) have gained substantial research interest due to their exceptional sensing capabilities. Traditionally, FBG fabrication has required the use of pre-hydrogenated fibers and high-cost laser systems such as excimer lasers at 193 nm or femtosecond lasers. In this study, we present the first instance of FBG inscription in hydrogen-loaded, standard single-mode silica optical fibers using a more affordable 266 nm solid-state pulsed laser combined with a scanning phase mask lithography technique. We systematically explored the effects of pulse energy and scanning speed on the quality and spectral characteristics of the gratings, achieving reflectivities as high as 99.81%. Additionally, we tracked the spectral evolution during the FBG inscription process, demonstrating uniform growth of the core mode. We also investigated the stability of the core mode during a 24-h thermal annealing process up to 150 °C. The sensitivity was 10.7 pm/°C in the range of 0 to 130 °C. Furthermore, strain measurement was conducted based on the FBG annealed at 100 °C, showing a sensitivity of 0.943 pm/µε in the range of 0 to 1667 µε. Full article
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<p>Experimental setup for the inscription of FBGs using 266 nm solid-state laser pulses.</p>
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<p>Photo-induced transmitted spectra of FBGs inscribed with different pulse energies (1.75 mJ, 2 mJ, 2.2 mJ, 2.5 mJ) at a constant scanning speed of 0.012 mm/s and a pulse repetition rate of 20 Hz.</p>
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<p>Photo-induced reflected spectra of FBGs inscribed with different pulse energies (1.75 mJ, 2 mJ, 2.2 mJ, and 2.5 mJ) at a constant scanning speed of 0.012 mm/s and a pulse repetition rate of 20 Hz.</p>
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<p>Photo-induced transmitted spectra of FBGs inscribed with varying pulse energies (1.5 mJ, 1.75 mJ, 2 mJ, and 2.2 mJ) at a constant scanning speed of 0.01 mm/s and a pulse repetition rate of 20 Hz.</p>
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<p>The microscopic images of the fibers with different pulse energies (<b>a</b>) 1.5 mJ, (<b>b</b>) 1.75 mJ, (<b>c</b>) 2 mJ, and (<b>d</b>) 2.2 mJ at a constant scanning speed of 0.01 mm/s and a pulse repetition rate of 20 Hz.</p>
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<p>Photo-induced reflected spectra of FBGs inscribed with varying pulse energies (1.5 mJ, 1.75 mJ, 2 mJ, and 2.2 mJ) at a constant scanning speed of 0.01 mm/s and a pulse repetition rate of 20 Hz.</p>
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<p>Photo-induced transmitted spectra of FBGs inscribed at different scanning speeds (0.005 mm/s, 0.008 mm/s, 0.01 mm/s, 0.012 mm/s, and 0.015 mm/s) with a constant pulse energy of 1.75 mJ and a pulse repetition rate of 20 Hz.</p>
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<p>Photo-induced reflected spectra of FBGs inscribed at different scanning speeds (0.005 mm/s, 0.008 mm/s, 0.01 mm/s, 0.012 mm/s, and 0.015 mm/s) with a constant pulse energy of 1.75 mJ and a pulse repetition rate of 20 Hz.</p>
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<p>Growth of photo-induced FBG transmitted spectra as a function of inscription time, with a scanning speed of 0.008 mm/s, pulse energy of 1.75 mJ, and a pulse repetition rate of 20 Hz.</p>
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<p>Evolution of the FBG inscribed under conditions (0.008 mm/s, 1.75 mJ, 20 Hz) during the annealing process at 100 °C, showing (<b>a</b>) the Bragg wavelength shift and (<b>b</b>) the transmission depth of the core mode.</p>
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<p>Spectral comparison of FBGs inscribed under conditions (0.008 mm/s, 1.75 mJ, 20 Hz) before and after the annealing process.</p>
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<p>Transmitted amplitude spectrum evolution of the core mode as a function of temperature.</p>
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<p>Linear fit of the central wavelength evolution of the core mode as a function of temperature.</p>
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<p>Evolution of FBG inscribed under conditions (0.008 mm/s, 1.75 mJ, 20 Hz) during the annealing process at 150 °C, showing (<b>a</b>) the Bragg wavelength shift and (<b>b</b>) the transmission depth of the core mode.</p>
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<p>Transmitted amplitude spectrum evolution of the core mode as a function of temperature within the range of 0 to 130 °C.</p>
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<p>Linear fit of the central wavelength evolution of the core mode as a function of temperature within the range of 0 to 130 °C.</p>
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<p>Linear fit of the central wavelength evolution of the core mode as a function of strain.</p>
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12 pages, 4110 KiB  
Article
Wavelength Locking and Calibration of Fiber-Optic Ultrasonic Sensors Using Single-Sideband-Modulated Laser
by Mohammed Alshammari and Ming Han
Photonics 2024, 11(11), 1063; https://doi.org/10.3390/photonics11111063 - 13 Nov 2024
Viewed by 421
Abstract
Implementation of edge-filter detection for interrogating optical interferometric ultrasonic sensors is often hindered by the lack of cost-effective laser sources with agile wavelength tunability and good noise performance. The detected signal can also be affected by optical power variations and locking-point drift, negatively [...] Read more.
Implementation of edge-filter detection for interrogating optical interferometric ultrasonic sensors is often hindered by the lack of cost-effective laser sources with agile wavelength tunability and good noise performance. The detected signal can also be affected by optical power variations and locking-point drift, negatively affecting the sensor accuracy. Here, we report the use of laser single-sideband generation with a dual-parallel Mach–Zehnder interferometer (DP-MZI) for laser wavelength tuning and locking in edge-filter detection of fiber-optic ultrasonic sensors. We also demonstrate real-time in situ calibration of the sensor response to ultrasound-induced wavelength shift tuning. The DP-MZI is employed to generate a known wavelength modulation of the laser, whose response is used to gauge the sensor response to the ultrasound-induced wavelength shifts in real time and in situ. Experiments were performed on a fiber-optic ultrasonic sensor based on a high-finesse Fabry–Perot interferometer formed by two fiber Bragg gratings. The results demonstrated the effectiveness of the laser locking against laser wavelength drift and temperature variations and the effectiveness of the calibration method against optical power variations and locking-point drift. These techniques can enhance the operational robustness and increase the measurement accuracy of optical ultrasonic sensors. Full article
(This article belongs to the Special Issue Recent Research on Optical Sensing and Precision Measurement)
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Figure 1
<p>Schematics of (<b>a</b>) the proposed fiber-optic ultrasonic sensor system with edge-filter detection and real-time in situ calibration and (<b>b</b>) the single-sideband generation module. (<b>c</b>) Illustration of laser wavelength locking for ultrasound detection and laser wavelength modulation for calibration.</p>
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<p>(<b>a</b>) Schematic of the experimental setup. (<b>b</b>) Measured reflection spectrum of the sensor.</p>
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<p>Locking the single sideband to the spectral slope of the sensor against laser wavelength variation. (<b>a</b>) Sinusoidal laser wavelength modulation with a peak-to-peak wavelength shift of 12 pm, (<b>b</b>) recorded sensor system output in response to the ultrasound (<span class="html-italic">i<sub>s</sub></span>), (<b>c</b>) error signal of the feedback control loop, (<b>d</b>) the output from the controller that feeds the VCO, and (<b>e</b>) a detailed view of the ultrasound signals (<span class="html-italic">i<sub>s</sub></span>) obtained at the three operating points indicated in with (i), (ii), and (iii) (<b>b</b>).</p>
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<p>Results when the feedback control loop was open. (<b>a</b>) Sinusoidal laser wavelength modulation with a peak-to-peak wavelength shift of 12 pm. (<b>b</b>) Recorded sensor system output in response to the ultrasound (<span class="html-italic">i<sub>s</sub></span>), (<b>c</b>) error signal of the feedback control loop, (<b>d</b>) the output from the controller that feeds the VCO, and (<b>e</b>) a detailed view of the ultrasound signals (<span class="html-italic">i<sub>s</sub></span>) obtained at the three operating points indicated with (i), (ii), and (iii) in (<b>b</b>).</p>
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<p>Locking the single sideband to the spectral slope of the sensor against thermal-induced wavelength shift of the sensor. (<b>a</b>) Recorded sensor system output in response to the ultrasound (<span class="html-italic">i<sub>s</sub></span>), (<b>b</b>) error signal of the feedback control loop, (<b>c</b>) the output from the controller that feeds the VCO, and (<b>d</b>) a detailed view of the ultrasound signals (<span class="html-italic">i<sub>s</sub></span>) obtained at the five operating points indicated with (i), (ii), (iii), (iv) and (v) in (<b>a</b>).</p>
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<p>Results when the feedback control loop was open. (<b>a</b>) Recorded sensor system output in response to the ultrasound (<span class="html-italic">i<sub>s</sub></span>); (<b>b</b>) error signal of the feedback control loop; (<b>c</b>) the output from the controller that feeds the VCO; and (<b>d</b>) a detailed view of the ultrasound signals (<span class="html-italic">i<sub>s</sub></span>) obtained at the five operating points indicated with (i), (ii),(iii), (iv) and (v) in (<b>a</b>), showing large variations in amplitude.</p>
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<p>Results for demonstration of sensor calibration. (<b>a</b>) Recorded sensor system output in response to the ultrasound (<span class="html-italic">i<sub>s</sub></span>); (<b>b</b>) calibration signal (<span class="html-italic">ic</span>); (<b>c</b>) error signal of the feedback control; (<b>d</b>) controller output that feeds the VCO; (<b>e</b>) 50 mVpp 1 kHz modulation signal for generating the calibration; (<b>f</b>) detailed view of the ultrasound signals, <span class="html-italic">i<sub>s</sub></span> (blue), and calibration signal, <span class="html-italic">i<sub>c</sub></span> (red), obtained at the three operating points indicated in (<b>a</b>); and (<b>g</b>) the corresponding signals after calibration.</p>
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18 pages, 3382 KiB  
Article
Deep Learning-Enabled De-Noising of Fiber Bragg Grating-Based Glucose Sensor: Improving Sensing Accuracy of Experimental Data
by Harshit Tiwari, Yogendra S. Dwivedi, Rishav Singh, Anuj K. Sharma, Ajay Kumar Sharma, Richa Krishna, Nitin Singh Singha, Yogendra Kumar Prajapati and Carlos Marques
Photonics 2024, 11(11), 1058; https://doi.org/10.3390/photonics11111058 - 12 Nov 2024
Viewed by 537
Abstract
This paper outlines the successful utilization of deep learning (DL) techniques to elevate data quality for assessing Au-TFBG (tilted fiber Bragg grating) sensor performance. Our approach involves a well-structured DL-assisted framework integrating a hierarchical composite attention mechanism. In order to mitigate high variability [...] Read more.
This paper outlines the successful utilization of deep learning (DL) techniques to elevate data quality for assessing Au-TFBG (tilted fiber Bragg grating) sensor performance. Our approach involves a well-structured DL-assisted framework integrating a hierarchical composite attention mechanism. In order to mitigate high variability in experimental data, we initially employ seasonal decomposition using moving averages (SDMA) statistical models to filter out redundant data points. Subsequently, sequential DL models extrapolate the normalized transmittance (Tn) vs. wavelength spectra, which showcases promising results through our SpecExLSTM model. Furthermore, we introduce the AttentiveSpecExLSTM model, integrating a composite attention mechanism to improve Tn sequence prediction accuracy. Evaluation metrics demonstrate its superior performance, including a root mean square error of 1.73 ± 0.05, a mean absolute error of 1.20 ± 0.04, and a symmetric mean absolute percentage error of 2.22 ± 0.05, among others. Additionally, our novel minima difference (Min. Dif.) metric achieves a value of 1.08 ± 0.46, quantifying wavelength for the global minima within the Tn sequence. The composite attention mechanism in the AttentiveSpecExLSTM adeptly captures both high-level and low-level dependencies, refining the model’s comprehension and guiding informed decisions. Hierarchical dot and additive attention within this model enable nuanced attention refinement across model layers; dot attention focuses on high-level dependencies, while additive attention fine-tunes its focus on low-level dependencies within the sequence. This innovative strategy enables accurate estimation of the spectral width (full-width half maxima) of the Tn curve, surpassing raw data’s capabilities. These findings significantly contribute to data quality enhancement and sensor performance analysis. Insights from this study hold promise for future sensor applications, enhancing sensitivity and accuracy by improving experimental data quality and sensor performance assessment. Full article
(This article belongs to the Special Issue Optical Fiber Sensors: Recent Progress and Future Prospects)
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<p>(<b>a</b>) Au-TFBG data for days 1–3 with varying glucose levels; <span class="html-italic">X</span>-axis: λ (in nm); <span class="html-italic">Y</span>-axis: T<sub>n</sub>. (<b>b</b>) Reduced variability in Au-TFBG for days 1–3 using SDMA across glucose levels.</p>
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<p>High-level representations of the <span class="html-italic">AttentiveSpecExLSTM</span> model for improving spectral width estimations, where inputs sequence represents the wavelength sequence with one-hot encoded day vector. The model contains four layers with a hierarchical attention architecture.</p>
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<p>Relationship between trans. minima and glucose concentration over time. The graph demonstrates a consistent λ (units in nanometers or nm) value corresponding to each trans. minima, indicating a stable correlation between glucose concentration and the trans. minima. For day 1, the two different sensor readings of trans. minima for a given concentration (shown in subplots (<b>a</b>,<b>b</b>)) highlight the reliability of this parameter in assessing glucose levels. This consistency is similarly observed for day 2 and day 3, as reflected in subplots (<b>c</b>–<b>f</b>), respectively.</p>
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<p><span class="html-italic">SpecExLSTM</span> (<b>a</b>–<b>f</b>) and <span class="html-italic">AttentiveSpecExLSTM</span> (<b>g</b>–<b>l</b>) models’ re-constructed predictions on the test data split. The <span class="html-italic">x</span>-axis in the subplots represents λ in nm.</p>
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<p>Attention maps with respect to dynamic changes in the temporal dimension of the ablated model: (<b>a</b>) L1-Dot Attn. only; (<b>b</b>) L1-Add Attn. only; (<b>c</b>) L2-Dot Attn. only; (<b>d</b>) L2-Add Attn. only; (<b>e</b>) Both-Dot Attn.; (<b>f</b>) Both-Add Attn.; (<b>g</b>) L1-Add/L2- Dot Attn;, and (<b>f</b>) L1-Dot/L2- Add Attn. The <span class="html-italic">x</span>-axis in the subplots (<b>a</b>–<b>h</b>) represents λ in nm. The attention maps in the subplots’ x- and <span class="html-italic">y</span>-axes represent the number of attention units. The sub-subfigures (i–iv) in the subfigures represent the attention maps for the respective temporal range (highlighted with a red line) in the subfigures.</p>
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<p>FWHM calculation for day 1 without extrapolation for Cg of 1% (<span class="html-italic">x</span>-axis represents λ in nm).</p>
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<p>FWHM measurement after extrapolating left-bound (<span class="html-italic">x</span>-axis represents λ in nm).</p>
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14 pages, 4903 KiB  
Article
Fiber-Optic Sensor Spectrum Noise Reduction Based on a Generative Adversarial Network
by Yujie Lu, Qingbin Du, Ruijia Zhang, Bo Wang, Zigeng Liu, Qizhe Tang, Pan Dai, Xiangxiang Fan and Chun Huang
Sensors 2024, 24(22), 7127; https://doi.org/10.3390/s24227127 - 6 Nov 2024
Viewed by 483
Abstract
In the field of fiber-optic sensing, effectively reducing the noise of sensing spectra and achieving a high signal-to-noise ratio (SNR) has consistently been a focal point of research. This study proposes a deep-learning-based denoising method for fiber-optic sensors, which involves pre-processing the sensor [...] Read more.
In the field of fiber-optic sensing, effectively reducing the noise of sensing spectra and achieving a high signal-to-noise ratio (SNR) has consistently been a focal point of research. This study proposes a deep-learning-based denoising method for fiber-optic sensors, which involves pre-processing the sensor spectrum into a 2D image and training with a cycle-consistent generative adversarial network (Cycle-GAN) model. The pre-trained algorithm demonstrates the ability to effectively denoise various spectrum types and noise profiles. This study evaluates the denoising performance of simulated spectra obtained from four different types of fiber-optic sensors: fiber Fabry–Perot interferometer (FPI), regular fiber Bragg grating (FBG), chirped FBG, and FBG pair. Compared to traditional denoising algorithms such as wavelet transform (WT) and empirical mode decomposition (EMD), the proposed method achieves an SNR improvement of up to 13.71 dB, an RMSE that is up to three times smaller, and a minimum correlation coefficient (R2) of no less than 99.70% with the original high-SNR signals. Additionally, the proposed algorithm was tested for multimode noise reduction, demonstrating an excellent linearity in temperature response with a R2 of 99.95% for its linear fitting and 99.74% for the temperature response obtained from single-mode fiber sensors. The proposed denoising approach effectively reduces the impact of various noises from the sensing system, enhancing the practicality of fiber-optic sensing, especially for specialized fiber applications in research and industrial domains. Full article
(This article belongs to the Special Issue New Prospects in Fiber Optic Sensors and Applications)
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<p>(<b>a</b>) The structure of a regular FBG; (<b>b</b>) a normalized FBG spectrum obtained from simulation, and (<b>c</b>) its reshaped 2D image.</p>
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<p>Cycle-GAN denoising flow chart for a fiber-optic sensor spectrum.</p>
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<p>Simulation of high-SNR and noise-added spectra of (<b>a</b>) regular low-finesse FPI; (<b>b</b>) regular FBG; (<b>c</b>) chirped FBG; and (<b>d</b>) FBG pair sensors. The corresponding reshape gray-level image is on the right side of each spectrum.</p>
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<p>Setup of the FPI sensor’s modal noise reduction.</p>
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<p>Silicon wafer FPI spectrum with (<b>a</b>) SMF and (<b>b</b>) MMF as the lead-in fiber.</p>
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<p>Cycle-GAN-based algorithm denoising results of (<b>a</b>) regular low-finesse FPI; (<b>b</b>) regular FBG; (<b>c</b>) chirped FBG; and (<b>d</b>) FBG pair sensors. For each sensor, the top half is the denoised spectrum and the bottom half is the difference from the high-SNR spectrum.</p>
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<p>(<b>a</b>) The original MMF-FPI spectrum and its denoised output from the Cycle-GAN-based algorithm; the 2D reshaped image of (<b>b</b>) the original MMF-FPI spectrum; (<b>c</b>) the denoised spectrum.</p>
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<p>(<b>a</b>) Wavelength shift versus temperature for the denoised FPI; (<b>b</b>) wavelength shift versus temperature for SMF and denoised FPI.</p>
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<p>(<b>a</b>) Comparison of spectrum of MMF-FPI and noise-reduced spectra obtained via Cycle-GAN-based algorithm and low-pass filter; (<b>b</b>) wavelength shift versus temperature for MMF-FPI with LPF and its linear fit; (<b>c</b>) wavelength shift versus temperature for SMF and MMF-FPI with LPF.</p>
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15 pages, 5629 KiB  
Article
FBG and BOTDA Based Monitoring of Mine Pressure Under Remaining Coal Pillars Using Physical Modeling
by Dingding Zhang, Zhi Li, Yanyan Duan, Long Yang and Hongrui Liu
Sensors 2024, 24(21), 7037; https://doi.org/10.3390/s24217037 - 31 Oct 2024
Viewed by 400
Abstract
Strong mine pressure often emerges when the working face of the lower coal seam in a closely spaced coal seam system passes through the remaining coal pillar in the overlying goaf. This study investigates the law of overburden movement and the manifestation of [...] Read more.
Strong mine pressure often emerges when the working face of the lower coal seam in a closely spaced coal seam system passes through the remaining coal pillar in the overlying goaf. This study investigates the law of overburden movement and the manifestation of mine pressure during mining under the remaining coal pillar. A physical model measuring 2.5 × 0.2 × 1.503 m is constructed. Fiber Bragg grating sensing technology (FBG) and Brillouin optical time domain analysis technology (BOTDA) are employed in the physical model experiment to monitor the internal strain of the overlying rock as the working face advances. This study determines the laws of overlying rock fracture and working face pressure while mining coal seams beneath the remaining coal pillar. It analyzes the relationship between the pressure at the working face and the strain characteristics of the horizontally distributed optical fiber. A fiber grating characterization method is established for the stress evolution law of overlying rock while passing the remaining coal pillar. The experimental results indicated that the fracture angle of overlying rock gradually decreases during the mining stage through and after the coal pillar. In the mining stage through the coal pillar, the cycle pressure step distance of the working face is reduced by 33.3% compared to the stage after mining through the coal pillar. Initially, the strain pattern of the horizontal optical fiber is unimodal when pressure is first applied to the working face, and it transitions from unimodal to bimodal during periodic pressure. The peak value of fiber Bragg grating compressive strain and the range of influence of advanced support pressure are 3.6 times and 4.8 times, respectively, before passing through the remaining coal pillar. Finally, the accuracy of the FBG characterization method is verified by comparing it to the monitoring curve of the coal seam floor pressure sensor. The research results contribute to applying fiber optic sensing technology in mining physical model experiments. Full article
(This article belongs to the Special Issue Optical Sensors for Industrial Applications)
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<p>Monitoring principle of BOTDA.</p>
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<p>Physical model lithology distribution and sensor layout.</p>
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<p>The collapse form of overlying rock after 1<sup>−2</sup> coal seam mining.</p>
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<p>Characteristics of overlying rock collapse as the working face advances.</p>
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<p>DFOS strain curve before mining through coal pillar. (<b>a</b>) Advance from 500 to 1000 mm; (<b>b</b>) Overlying rock collapse characteristics when advancing 850 mm.</p>
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<p>DFOS strain curve before mining through coal pillar. (<b>a</b>) Advance from 110 to 1250 mm; (<b>b</b>) Overlying rock collapse characteristics when advancing 1250 mm.</p>
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<p>DFOS strain curve after mining through coal pillar. (<b>a</b>) Advance from 1350 to 2300 mm; (<b>b</b>) Overlying rock collapse characteristics when advancing 1450 mm.</p>
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<p>FBG strain changes during the process of advancing the working face.</p>
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<p>FBG test results and their corresponding relationship with the position of the remaining coal pillar.</p>
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<p>Comparison of monitoring curves between FBG and CFP as the working face advances.</p>
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15 pages, 6448 KiB  
Article
A Safe Fiber-Optic-Sensor-Assisted Industrial Microwave-Heating System
by Kivilcim Yüksel, Oguz Deniz Merdin, Damien Kinet, Murat Merdin, Corentin Guyot and Christophe Caucheteur
Sensors 2024, 24(21), 6995; https://doi.org/10.3390/s24216995 - 30 Oct 2024
Viewed by 448
Abstract
Industrial microwave-heating systems are pivotal in various sectors, including food processing and materials manufacturing, where precise temperature control and safety are critical. Conventional systems often struggle with uneven heat distribution and high fire risks due to the intrinsic properties of microwave heating. In [...] Read more.
Industrial microwave-heating systems are pivotal in various sectors, including food processing and materials manufacturing, where precise temperature control and safety are critical. Conventional systems often struggle with uneven heat distribution and high fire risks due to the intrinsic properties of microwave heating. In this work, a fiber-optic-sensor-assisted monitoring system is presented to tackle the pressing challenges associated with uneven heating and fire hazards in industrial microwave systems. The core innovation lies in the development of a sophisticated fiber-optic 2D temperature distribution sensor and a dedicated fire detector, both designed to significantly mitigate risks and optimize the heating process. Experimental results set the stage for future innovations that could transform the landscape of industrial heating technologies toward better process quality. Full article
(This article belongs to the Section Optical Sensors)
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<p>Block diagram of the sensor-assisted microwave-heating system.</p>
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<p>Schematic representation of sensor calibration setup.</p>
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<p>Variation in temperature measured using reference probes and FBG sensors (both with and without package) during a temperature cycle (from room temperature to 80 °C) for FBG#8 (<b>a</b>) and FBG#10 (<b>b</b>). Variation in the Bragg peak position as a function of the temperature for FOSAS-4 (having PTFE package), FBG#8, FBG#10 (<b>c</b>), and FOSAS-4 all 16 FBGs (<b>d</b>).</p>
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<p>Photo showing the setup for the functional tests of the IR detector. (<b>left</b>): direct exposure, (<b>right</b>): angled exposure. The distance between the sensor and the IR source is varied between 15 cm and 1 m.</p>
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<p>IR detector response: (<b>left</b>): Bragg wavelength shift (BWS), (<b>right</b>): Bragg wavelength difference (BWD). Time of exposure is varied between 1 s and 10 s.</p>
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<p>Manufactured casing for fire sensor.</p>
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<p>Mechanical design and the manufactured cavity.</p>
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<p>Measurement setup with the instrumented microwave oven on the left and the BSI-116 data acquisition system on the right.</p>
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<p>(<b>a</b>) Position of veins; (<b>b</b>) marble heating (a temperature difference up to 57 °C was observed between the hot spots of marble’s natural veins and the marble’s white parts). The cavity was 1500 mm × 1500 mm.</p>
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<p>(New cavity/old cavity) 2D heating-difference results (<b>a</b>) at 30 s and (<b>b</b>) at 360 s. The cavity is 1500 mm × 1500 mm.</p>
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<p>(New cavity—old cavity) 3D heating-difference results (<b>a</b>) at 30 s and (<b>b</b>) at 360 s.</p>
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<p>Fire sensor (S) and test fire location (F). (The oven cavity is divided into 5 × 5 grids of equal surface areas). (<b>a</b>) Fire at maximum distance; (<b>b</b>) aligned fire test.</p>
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14 pages, 5658 KiB  
Article
A New Type of Dynamic Vibration Fiber Sensor
by I-Nan Chang, Chih-Chuan Chiu and Wen-Fung Liu
Sensors 2024, 24(21), 6973; https://doi.org/10.3390/s24216973 - 30 Oct 2024
Viewed by 393
Abstract
A new-type vibration sensor based on a fiber Bragg grating combined with a special structure-packaged design is proposed for monitoring the mechanical vibration signals. Three different sensing structures, including the film squeeze type, new film squeeze type, and elastic tape squeeze type are [...] Read more.
A new-type vibration sensor based on a fiber Bragg grating combined with a special structure-packaged design is proposed for monitoring the mechanical vibration signals. Three different sensing structures, including the film squeeze type, new film squeeze type, and elastic tape squeeze type are proposed for measuring the vibration signals with the frequency range from tens to thousands of Hz. In the comparison to experimental results, the new film squeeze structure has a nice sensing performance in the range from 100 to 1000 Hz with a sensitivity of 0.302 mV/g. For the elastic tape squeeze structure, the elastic tape is designed to encapsulate the optical fiber with a good frequency response from 1100 to 3100 Hz. In addition, by using the new film squeeze structure to measure the steady-state and non-steady-state vibration signals, the spectral components of sensing signals are analyzed by using the wavelet transformation for confirming the testing signals. These vibration fiber sensors can be applied in the measurement of high-end manufacture-facility vibration or earthquake vibrations etc. Full article
(This article belongs to the Special Issue High-Resolution Guided-Wave Optical Sensors)
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<p>The cross-section of the package structure without the excitation of vibration signals.</p>
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<p>The 3D view and cross-section of the new film squeeze structure.</p>
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<p>Experimental configuration of generating vibration signals.</p>
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<p>Frequency response of bare fiber grating for sensing vibrational signals.</p>
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<p>Experimental set-up of sensing vibrational signals.</p>
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<p>The overlapping reflection spectra between the sensing grating and the matched grating.</p>
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<p>(<b>a</b>) 100 Hz sensing signal, (<b>b</b>) 300 Hz sensing signal, (<b>c</b>) 1000 Hz sensing signal.</p>
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<p>Comparison of frequency response of film squeeze type and bare fiber grating.</p>
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<p>(<b>a</b>) 100 Hz sensing signal, (<b>b</b>) 400 Hz sensing signal, (<b>c</b>) 2000 Hz sensing signal, (<b>d</b>) 3100 Hz sensing signal.</p>
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<p>Comparison of frequency response of elastic tape squeeze structure and unstructured fiber grating.</p>
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<p>The cross-section of elastic-tape squeeze type with a probe.</p>
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<p>The sensing signal of 10 Hz and sensing signal of 500 Hz.</p>
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<p>Comparison of frequency response of new film squeeze and unstructured fiber grating.</p>
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<p>The sensing signals with different vibration amplitude and frequency. (<b>a</b>) 220 Hz sensing signal vs 300 mV vibration amplitude, (<b>b</b>) 220 Hz sensing signal vs 100 mV vibration amplitude, (<b>c</b>) 500 Hz sensing signal vs 300 mV vibration amplitude, (<b>d</b>) 900 Hz sensing signal vs 300 mV vibration amplitude.</p>
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<p>The relationship between vibration signal and sensing amplitude.</p>
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<p>A signal frequency varies with time series (100~300 Hz).</p>
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<p>The time-frequency analysis of vibration signals with FFT.</p>
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<p>The time-frequency analysis of vibration signals with CWT.</p>
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10 pages, 8608 KiB  
Article
Large Range Curvature Measurement Using FBGs in Two-Core Fiber with Protective Coating
by Ruibin Chen, Lutian Li, Qianqing Yu, Zhijun Luo, Zhenggang Lian, Chuanxin Teng, Hang Qu and Xuehao Hu
Micromachines 2024, 15(11), 1310; https://doi.org/10.3390/mi15111310 - 28 Oct 2024
Viewed by 546
Abstract
In this work, we propose a fiber Bragg grating (FBG)-based sensor for curvature measurements. Two gratings are inscribed through the protective coating in a specialty optical fiber using focused femtosecond laser pulses and point-by-point direct writing technology. One grating is inscribed on the [...] Read more.
In this work, we propose a fiber Bragg grating (FBG)-based sensor for curvature measurements. Two gratings are inscribed through the protective coating in a specialty optical fiber using focused femtosecond laser pulses and point-by-point direct writing technology. One grating is inscribed on the central core adjacent to an air channel, while the other is inscribed on the eccentric core. The bending characteristics of the two-core fiber strongly depend on the bending direction due to the asymmetry of the fiber cores. A bending sensitivity of 58 pm/m1 is achieved by the FBG in the eccentric fiber core over the curvature range of 0–50 m1. Temperature and humidity cross-sensitivity could be significantly reduced by analyzing the differences in peak shifts between the two gratings. The sensor features a large sensing range and good robustness due to the presence of its protective buffer coating, which makes it a good candidate for curvature sensing in engineering fields. Full article
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<p>(<b>a</b>) Microscopic image of the fiber cross section. (<b>b</b>) Microscopic image showing the FBGs PbP-inscribed by the femeosecond laser with a wavelength of 520 nm.</p>
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<p>Reflected spectrum of the two FBGs in the eccentric and central core of the specialty fiber.</p>
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<p>(<b>a</b>) Schematic of the experimental set-up for testing bending characteristics; (<b>b</b>) illustration of the fiber bending in 0° orientation; (<b>c</b>) illustration of four fiber orientations (0°, 90°, 180°, and 270°).</p>
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<p>(<b>a</b>) The reflected spectrum of the sensor with different curvatures, when the specialty fiber is in the 0° orientation. (<b>b</b>) The resonant wavelength dependence on the curvatures for the 0°, 90°,180° and 270° fiber orientations.</p>
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<p>(<b>a</b>) Characterization of the thermal stability of the sensor and the difference in spectral shifts of the two FBGs due to temperature variations; (<b>b</b>) Characterization of the humidity stability of the sensor and the difference in spectral shift of the two FBGs due to humidity variations.</p>
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<p>(<b>a</b>) Reflection spectra of the fiber sensor as the curvature increased from 0 to ~210 m<sup>−1</sup>, (<b>b</b>) spectral shifts of the FBGs in the central core and the eccentric core, (<b>c</b>) variations in the FWHM and the amplitude of the reflection peak.</p>
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11 pages, 5544 KiB  
Communication
Phase-Shifted Fiber Bragg Grating by Selective Pitch Slicing
by Paulo Robalinho, Vinícius Piaia, Liliana Soares, Susana Novais, António Lobo Ribeiro, Susana Silva and Orlando Frazão
Sensors 2024, 24(21), 6898; https://doi.org/10.3390/s24216898 - 28 Oct 2024
Viewed by 524
Abstract
This paper presents a new type of phase-shifted Fiber Bragg Grating (FBG): the sliced-FBG (SFBG). The fabrication process involves cutting a standard FBG inside its grating region. As a result, the last grating pitch is shorter than the others. The optical output signal [...] Read more.
This paper presents a new type of phase-shifted Fiber Bragg Grating (FBG): the sliced-FBG (SFBG). The fabrication process involves cutting a standard FBG inside its grating region. As a result, the last grating pitch is shorter than the others. The optical output signal consists of the overlap between the FBG reflection and the reflection at the fiber-cleaved tip. This new fiber optic device has been studied as a vibration sensor, allowing for the characterization of this sensor in the frequency range of 150 Hz to 70 kHz. How the phase shift in the FBG can be controlled by changing the length of the last pitch is also shown. This device can be used as a filter and a sensing element. As a sensing element, we will demonstrate its application as a vibration sensor that can be utilized in various applications, particularly in monitoring mechanical structures. Full article
(This article belongs to the Section Optical Sensors)
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<p>SFBG manufacturing scheme.</p>
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<p>The graphical representation of Equation (3) simulation for: (<b>a</b>) <span class="html-italic">L</span><sub>Φ</sub> = 0, <span class="html-italic">L</span><sub>Φ</sub> = <span class="html-italic">L</span><sub>Λ</sub>/4, (<b>b</b>) <span class="html-italic">L</span><sub>Φ</sub> = <span class="html-italic">L</span><sub>Λ</sub>/2, (<b>c</b>) <span class="html-italic">L</span><sub>Φ</sub> = 3<span class="html-italic">L</span><sub>Λ</sub>/4.</p>
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<p>The spectrum of FBG structure: (<b>a</b>) before the cut and (<b>b</b>) after the cut.</p>
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<p>(<b>a</b>) Scheme used for the spectral analysis, (<b>b</b>) <span class="html-italic">L</span><sub>Φ</sub> &lt; <span class="html-italic">L</span><sub>Λ</sub>/2, (<b>c</b>) <span class="html-italic">L</span><sub>Φ</sub> = <span class="html-italic">L</span><sub>Λ</sub>/2 and (<b>d</b>) <span class="html-italic">L</span><sub>Φ</sub> &gt; <span class="html-italic">L</span><sub>Λ</sub>/2. These results were obtained from the SFBG, and the variation is due to the applied axial stress.</p>
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<p>(<b>a</b>) Scheme used for the spectral analysis, (<b>b</b>) <span class="html-italic">L</span><sub>Φ</sub> &lt; <span class="html-italic">L</span><sub>Λ</sub>/2, (<b>c</b>) <span class="html-italic">L</span><sub>Φ</sub> = <span class="html-italic">L</span><sub>Λ</sub>/2 and (<b>d</b>) <span class="html-italic">L</span><sub>Φ</sub> &gt; <span class="html-italic">L</span><sub>Λ</sub>/2. These results were obtained from the SFBG, and the variation is due to the applied axial stress.</p>
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<p>(<b>a</b>) Scheme for the FBG’s vibration characterization, (<b>b</b>) spectrum used for the measurement.</p>
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<p>(<b>a</b>) Scheme for the FBG’s vibration characterization, (<b>b</b>) spectrum used for the measurement.</p>
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<p>SNR versus frequency plots revealed a range of responses between 0.15 and 70 kHz. Below are the signals acquired by the photodetector when the oscillator oscillates at 230 Hz, 8200 Hz and 21 kHz and the corresponding Fourier transforms.</p>
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9 pages, 1515 KiB  
Article
Temperature and Lateral Pressure Sensing Using a Sagnac Sensor Based on Cascaded Tilted Grating and Polarization-Maintaining Fibers
by Yifan Liu, Yujian Li, Pin Xu and Changyuan Yu
Sensors 2024, 24(21), 6779; https://doi.org/10.3390/s24216779 - 22 Oct 2024
Viewed by 477
Abstract
This study introduces a Sagnac Interferometer (SI) fiber sensor that integrates Polarization-Maintaining Fibers (PMFs) with a Tilted Fiber Bragg Grating (TFBG) for the dual-parameter measurement of strain and lateral pressure. By incorporating a 6° TFBG with PMFs into the SI sensor, its sensitivity [...] Read more.
This study introduces a Sagnac Interferometer (SI) fiber sensor that integrates Polarization-Maintaining Fibers (PMFs) with a Tilted Fiber Bragg Grating (TFBG) for the dual-parameter measurement of strain and lateral pressure. By incorporating a 6° TFBG with PMFs into the SI sensor, its sensitivity is significantly enhanced, enabling advanced multi-parameter sensing capabilities. The sensor demonstrates a temperature sensitivity of −1.413 nm/°C and a lateral pressure sensitivity of −4.264 dB/kPa, as validated by repeated experiments. The results exhibit excellent repeatability and high precision, underscoring the sensor’s potential for robust and accurate multi-parameter sensing applications. Full article
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<p>(<b>a</b>) Structure of the core-to-core linking of TFBG and PMF. (<b>b</b>) Structure of the designed sensor.</p>
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<p>Transmission spectrum of SI combined with TFBG.</p>
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<p>Temperature measurement experiment.</p>
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<p>(<b>a</b>) Obtained transmission spectrum, (<b>b</b>) spectrum at 47 °C, (<b>c</b>) detailed graph of peak 1, and (<b>d</b>) linear fit of temperature sensing. (<b>e</b>) Intensity change of Peak A with temperature variation).</p>
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<p>Lateral pressure measurement experiment.</p>
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<p>(<b>a</b>) Obtained transmission spectrum, (<b>b</b>) detailed graph of peak at 47 °C, and (<b>c</b>) linear fit of temperature sensing.</p>
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18 pages, 10716 KiB  
Article
A Novel FBG Placement Optimization Method for Tunnel Monitoring Based on WOA and Deep Q-Network
by Jiguo Liu, Ming Song, Heng Shu, Wenbo Peng, Longhai Wei and Kai Wang
Symmetry 2024, 16(10), 1400; https://doi.org/10.3390/sym16101400 - 21 Oct 2024
Viewed by 590
Abstract
By employing the whale optimization algorithm’s (WOA) capability to reduce the probability of being stuck in a locally optimal solution, this study proposed an improved WOA-DQN algorithm based on the Deep Q-Network algorithm (DQN). Firstly, the mathematical model of Fiber Bragg Grating (FBG) [...] Read more.
By employing the whale optimization algorithm’s (WOA) capability to reduce the probability of being stuck in a locally optimal solution, this study proposed an improved WOA-DQN algorithm based on the Deep Q-Network algorithm (DQN). Firstly, the mathematical model of Fiber Bragg Grating (FBG) sensor placement was established to calculate the reward of DQN. Secondly, the effectiveness and applicability of WOA-DQN were validated through experiments in nine cases. It indicated that the algorithm is far superior to other methods (Noisy DQN, Prioritized DQN, DQN, WOA), especially with the learning rate of 0.001, the initial noise 0.4, the hidden layer 3–512, and the updated frequency of 20. Finally, the FBG sensors were placed at [0°, 27°, 30°, 47°, 51°, 111°, 126°, 219°, 221°, 289°] to detect the accurate deformation of the tunnel with the maximum error 8.66 mm, which is better than the traditional placement. In conclusion, the algorithm provides a theoretical foundation for sensor placement and improves monitoring accuracy. It further shows great promise for deformation monitoring in tunnels. Full article
(This article belongs to the Section Computer)
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<p>Reconstruction of tunnel cross-section curve.</p>
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<p>Special cases of curve fitting.</p>
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<p>Flowchart of the WOA-DQN algorithm.</p>
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<p>Training process and total reward of Case 1.</p>
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<p>Tunnel reconstruction result of Case 1.</p>
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<p>Performance of different numbers of sensors in all cases.</p>
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<p>Final FBG sensors placement.</p>
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<p>Performance of different learning rates.</p>
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<p>Performance of different initial noise parameters.</p>
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<p>Performance of different hiding layer parameters.</p>
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<p>Performance of different updating frequencies.</p>
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<p>Performance of 5 algorithms in Case 1.</p>
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<p>Performance of 5 algorithms in all Cases.</p>
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<p>Performance of 5 algorithms in all Cases.</p>
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11 pages, 18597 KiB  
Article
Demodulating Optical Wireless Communication of FBG Sensing with Turbulence-Caused Noise by Stacked Denoising Autoencoders and the Deep Belief Network
by Shegaw Demessie Bogale, Cheng-Kai Yao, Yibeltal Chanie Manie, Amare Mulatie Dehnaw, Minyechil Alehegn Tefera, Wei-Long Li, Zi-Gui Zhong and Peng-Chun Peng
Electronics 2024, 13(20), 4127; https://doi.org/10.3390/electronics13204127 - 20 Oct 2024
Viewed by 776
Abstract
Free-space optics communication (FSO) can be used as a transmission medium for fiber optic sensing signals to make fiber optic sensing easier to implement; however, interference with the sensing signals caused by the optical turbulence and scattering of airborne particles in the FSO [...] Read more.
Free-space optics communication (FSO) can be used as a transmission medium for fiber optic sensing signals to make fiber optic sensing easier to implement; however, interference with the sensing signals caused by the optical turbulence and scattering of airborne particles in the FSO path is a potential problem. This work aims to deep denoise sensed signals from fiber Bragg grating (FBG) sensors based on FSO link transmission using advanced denoising deep learning techniques, such as stacked denoising autoencoders (SDAE). Furthermore, it will demodulate the sensed wavelength of FBGs by applying the deep belief network (DBN) technique. This is the first time the real FBG sensing experiment has utilized the actual noise interference caused by the environmental turbulence from an FSO link rather than adding noise through numerical processing. Consequently, the spectrum of the FBG sensors is clearly modulated by the noise and the issue with peak power variation. This complicates the determination of the center wavelengths of multiple stacked FBG spectra, requiring the use of machine learning techniques to predict these wavelengths. The results indicate that SDAE is efficient in denoising from the FBG spectrum, and DBN is effective in demodulating the central wavelength of the overlapped FBG spectrum. Thus, it is beneficial to implement an FSO link-based FBG sensing system in adverse weather conditions or atmospheric turbulence. Full article
(This article belongs to the Section Microwave and Wireless Communications)
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<p>Experimental framework for FBG array sensing based on FSO transmission with incidental particle scattering. The sensed data are used for AI model training and testing. (BLS: broadband light source; Cir.: circulator; OSA: optical spectrum analyzer; PC: personal computer).</p>
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<p>The corresponding values of the three FBG reflected wavelengths in each strain step.</p>
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<p>(<b>a</b>) Comparison of some FBG spectra before and after denoising; (<b>b</b>) Presentation of all FBG spectra (step 1 to step 16 in order) before and after denoising.</p>
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<p>Signal-to-noise ratio analysis (<b>a</b>) before SDAE denoising; (<b>b</b>) after SDAE denoising.</p>
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<p>The peak power of FBGs for each of the 19 spectra collected under strain steps 1, 8, and 16.</p>
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<p>Flowchart of wavelength demodulation by DBN.</p>
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<p>Parameters of the proposed SDAE and DBN models.</p>
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<p>Training efficiency of the DBN model in terms of accuracy and loss.</p>
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<p>Performance comparison with different machine learning models.</p>
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<p>(<b>a</b>) FBG peak wavelength prediction after applying SDAE and DBN models. (<b>b</b>) FBG peak wavelength prediction after applying the DBN model only.</p>
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