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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 253
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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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 404
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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16 pages, 16410 KiB  
Article
A Tunable and Switchable Multi-Wavelength Erbium-Doped Fiber Ring Laser Enabled by Adjusting the Spectral Fringe Visibility of a Mach-Zehnder Fiber Interferometer
by Romeo Emmanuel Nuñez Gomez, Gilberto Anzueto Sánchez, Alejando Martínez Ríos, Ariel Fong González, Alfredo Olarte Paredes, Areli Marlen Salgado Delgado, Jesús Castrellón Uribe and René Salgado Delgado
Appl. Sci. 2024, 14(21), 9846; https://doi.org/10.3390/app14219846 - 28 Oct 2024
Viewed by 824
Abstract
This paper presents a tunable, switchable multi-wavelength emission from an erbium-doped fiber ring laser, enabled by adjusting the spectral fringe visibility of a fiber interferometer filter. The filter is formed with specially designed concatenated tapered fibers to configure a Mach-Zehnder fiber interferometer (MZFI). [...] Read more.
This paper presents a tunable, switchable multi-wavelength emission from an erbium-doped fiber ring laser, enabled by adjusting the spectral fringe visibility of a fiber interferometer filter. The filter is formed with specially designed concatenated tapered fibers to configure a Mach-Zehnder fiber interferometer (MZFI). The laser emission is highly flexible and reconfigurable, allowing for tuning between single- and dual-wavelength operation. The laser can switch sequentially from one up to six wavelengths by fixing the curvature and adjusting the polarization state. The lasing emission is generated over a stable wavelength range between 1559.59 nm and 1563.54 nm, exhibiting an optical signal-to-noise ratio (OSNR) exceeding ~35 dB. The performance of amplitude and wavelength fluctuations were evaluated, indicating an appropriate stability of ~3 dB and a shift less than 0.1 nm within a 45 min period at room temperature. A detailed comparison with the literature is given. Full article
(This article belongs to the Special Issue Recent Trends in Fiber Optic Sensor: Technology and Applications)
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<p>Experimental erbium-doped fiber ring laser cavity setup for tunable and multi-wavelength emission.</p>
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<p>(<b>a</b>) MZFI structure formed with a pair of tapered sections fabricated on SMF-28, (<b>b</b>) displacement mechanism to used induce curvature in the MZFI.</p>
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<p>ASE spectrum as the light source from the EDF (black line) and the modified spectrum after passing through the MZFI (red line). The laser oscillation at 1563.07 nm is shown by the blue line.</p>
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<p>(<b>a</b>) The progressive modification of ASE spectrum with increasing curvature applied to the MZFI, (<b>b</b>) an inset in the range of 1541 to 1560 nm demonstrates an FSR of 5 nm.</p>
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<p>The wavelength shifts as a function of curvature (0 m<sup>−1</sup> to 2.93 m<sup>−1</sup>) and the variation of the measured fringe visibility.</p>
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<p>Tunable single laser wavelength between 1563.705 nm to 1558.05 nm for the curvatures from 0 m<sup>−1</sup> to 2.79 m<sup>−1</sup>.</p>
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<p>(<b>a</b>). Switchable dual-wavelength emissions generated at curvatures of 1.53 m<sup>−1</sup> with 1559.07 nm and 1563.66 nm, (<b>b</b>) 2.33 m<sup>−1</sup> with 1543.21 nm and 1549.287 nm, (<b>c</b>) 2.5 m<sup>−1</sup> with 1554.61 nm and 1559.667 nm, (<b>d</b>) 2.75 m<sup>−1</sup> with 1556.8 nm and 1561.877 nm.</p>
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<p>(<b>a</b>) Single-wavelength oscillation at 1562.22 nm, (<b>b</b>) dual-wavelength oscillation (1562.22–1562.875 nm), (<b>c</b>) triple-wavelength oscillation (1560.175–1562.22–1562.88 nm).</p>
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<p>(<b>a</b>) Quadruple-wavelength emission (1560.85–1561.51–1562.26–1562.86 nm), (<b>b</b>) quintuple-wavelength emission (1559.59–1560.91–1561.58–1562.93–1563.61 nm), and (<b>c</b>) sextuple-wavelength emission (1560.25–1560.97–1561.63–1562.29–1562.98–1563.64 nm).</p>
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<p>(<b>a</b>) Spectral distribution stability of a single laser oscillation at 1562.22 nm, with high-intensity uniformity across the spectrum, (<b>b</b>) a maximum wavelength shift of 0.01 nm, and (<b>c</b>) output power fluctuations of less than 0.12 dB.</p>
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<p>(<b>a</b>). Stability of the dual-wavelength laser oscillation at 1562.22–1562.785 nm with uniform intensity, (<b>b</b>) a maximum wavelength shift of 0.07 nm, and (<b>c</b>) output power fluctuations of less than 0.25 dB.</p>
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<p>(<b>a</b>) Power stability of the triple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.07 nm, and (<b>c</b>) maximum amplitude fluctuation of 0.51dB for the 1562.88 nm line.</p>
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<p>(<b>a</b>) Power stability of the quadruple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.22 nm, and (<b>c</b>) maximum amplitude fluctuation of 3 dB for the 1562.83 nm line.</p>
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<p>(<b>a</b>) Power stability of the quintuple-wavelength laser system, (<b>b</b>) maximum wavelength shift of 0.07 nm, and (<b>c</b>) maximum amplitude fluctuation of 1.7 dB for the 1561.58 nm line.</p>
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<p>(<b>a</b>) Power stability of the sextuple-wavelength laser system, (<b>b</b>) negligible wavelength shift, and (<b>c</b>) maximum amplitude fluctuation of 2.71 dB for the 1562.98 nm line.</p>
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12 pages, 2870 KiB  
Article
Highly Sensitive Gas Pressure Sensing with Temperature Monitoring Using a Slightly Tapered Fiber with an Inner Micro-Cavity and a Micro-Channel
by Changwei Sun, Fen Yu, Huifang Chen, Dongning Wang and Ben Xu
Sensors 2024, 24(21), 6844; https://doi.org/10.3390/s24216844 - 24 Oct 2024
Viewed by 443
Abstract
A highly sensitive optical fiber gas pressure sensor with temperature monitoring is proposed and demonstrated. It is based on a slightly tapered fiber with an inner micro-cavity forming an in-fiber Mach–Zehnder interferometer (MZI), and a micro-channel is drilled into the lateral wall of [...] Read more.
A highly sensitive optical fiber gas pressure sensor with temperature monitoring is proposed and demonstrated. It is based on a slightly tapered fiber with an inner micro-cavity forming an in-fiber Mach–Zehnder interferometer (MZI), and a micro-channel is drilled into the lateral wall of the in-fiber micro-cavity using a femtosecond laser to allow gas to flow in. Due to the dependence of the refractive index (RI) of air inside the micro-cavity on its gas pressure and the high RI sensitivity of the MZI, the device is extremely sensitive to gas pressure. To prevent fiber breakage, the MZI is housed in a silicate capillary tube with an air inlet. Multiple modes are excited by slightly tapering the inner micro-cavity, and the resonance dips in the sensor’s transmission spectrum feature different linear gas pressure and temperature responses, so a sensitivity matrix algorithm can be used to achieve simultaneous demodulation of two parameters, thus resolving the temperature crosstalk. As expected, the experimental results demonstrated the reliability of the matrix algorithm, with pressure sensitivity reaching up to ~−12.967 nm/MPa and temperature sensitivity of ~89 pm/°C. The features of robust mechanical strength and high air pressure sensitivity with temperature monitoring imply that the proposed sensor has good practical and application prospects. Full article
(This article belongs to the Section Optical Sensors)
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<p>Schematic diagram of the gas pressure sensor.</p>
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<p>The fabrication process of the gas pressure sensor. (<b>a</b>) A small pit is etched on the end face of the SMF by using Fs-laser. (<b>b</b>) The etched fiber is spliced to another SMF with a flat end face. (<b>c</b>) The fiber with an inner micro-cavity is tapered by streching. (<b>d</b>) A micro-channel is drilled in the lateral wall of the micro-cavity by using Fs-laser. (<b>e</b>) The fiber-in MZI is housed in a silicate capillary tube. (<b>f</b>) Microscopic image of the fiber-in MZI encapsulated in the capillary tube.</p>
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<p>Reflectance and transmission spectra monitored during the device preparation process. (<b>a</b>) The reflection and transmission spectra of the non-tapered device after the preparation steps corresponding to <a href="#sensors-24-06844-f002" class="html-fig">Figure 2</a>b. (<b>b</b>) Reflection and transmission spectra of the slightly tapered device before and after drilling the micro-channel.</p>
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<p>Strain response of the fiber-in MZI (<b>a</b>) Transmission spectra of the device under different strains and (<b>b</b>) dip wavelength shift versus strain.</p>
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<p>Experimental setup for investigating the response of the sensor to gas pressure.</p>
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<p>Pressure response of the sensor with capillary enveloped. (<b>a</b>) Transmission spectra of the sensor under different pressures; (<b>b</b>) dip wavelength shift versus gas pressure. Correlation between the resonance wavelength shift and the differential gas pressure.</p>
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<p>Temperature response of the fiber-in MZI. (<b>a</b>) Transmission spectra under different temperatures; (<b>b</b>) dip wavelength shift versus temperature.</p>
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<p>Reflection and transmission spectra of the second fiber-in MZI before and after drilling the micro-channel.</p>
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<p>Gas pressure response of the second sensor. (<b>a</b>) Reflection spectral of the sensor at different gas pressures, and (<b>b</b>) wavelength shifts of dip A and B versus differential gas pressure.</p>
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<p>Temperature response of the second sensor. (<b>a</b>) Reflection spectral of the sensor at different temperatures, and (<b>b</b>) wavelength shifts of dip A and B versus temperature.</p>
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<p>Results of simultaneous gas pressure and temperature.</p>
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12 pages, 11748 KiB  
Article
Wavelength-Switchable Ytterbium-Doped Mode-Locked Fiber Laser Based on a Vernier Effect Filter
by Hailong Xu, Liqiang Zhang, Xiangdong Li, Jiaxin Li, Yuanzhen Liu, Yicun Yao and Minghong Wang
Micromachines 2024, 15(11), 1289; https://doi.org/10.3390/mi15111289 - 23 Oct 2024
Viewed by 539
Abstract
A wavelength-switchable ytterbium-doped mode-locked fiber laser is reported in this article. Two Mach–Zehnder interferometers (MZIs, denoted as MZI1, MZI2) with close free spectral ranges (FSRs) are connected in series to form a Vernier effect sensor. By utilizing the filtering effect of the Vernier [...] Read more.
A wavelength-switchable ytterbium-doped mode-locked fiber laser is reported in this article. Two Mach–Zehnder interferometers (MZIs, denoted as MZI1, MZI2) with close free spectral ranges (FSRs) are connected in series to form a Vernier effect sensor. By utilizing the filtering effect of the Vernier effect sensor, the wavelength-switchable output of an ytterbium-doped mode-locked fiber laser is realized. When the 3 dB bandwidth of the Vernier effect filter is set to be 5.31 nm around 1073.42 nm, stable dissipative solitons are obtained. Stretching MZI1 horizontally, the central wavelengths of the pulses can be switched among 1073.42 nm, 1055.38 nm, and 1036.22 nm, with a total tunable central wavelength range of 37.2 nm. When the 3 dB bandwidth of the Vernier effect filter is set to be 4.07 nm, stable amplifier similaritons are obtained. Stretching MZI1 horizontally, the central wavelengths of the pulses are switchable among 1072.71 nm, 1060.15 nm, 1048.92 nm, and 1037.26 nm, with a total tunable central wavelength range of 35.15 nm. Compared with traditional fiber interference filters, the Vernier effect filter has a higher sensitivity, making wavelength switching more convenient and providing a wider tuning range for the ytterbium-doped mode-locked fiber laser. Full article
(This article belongs to the Special Issue High Power Fiber Laser Technology)
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<p>Calculated transmission cures of MZI1 (<b>a</b>) and MZI2 (<b>b</b>), and the superimposed spectra (<b>c</b>). The blue curves in (<b>b</b>,<b>c</b>) are the results of changing the optical path length of MZI2.</p>
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<p>Schematic diagram of the Vernier effect filter based on tapered SCF MZIs.</p>
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<p>(<b>a</b>,<b>b</b>) Transmission curves of MZI1 and MZI2 with different FSRs. (<b>c</b>,<b>d</b>) Superimposed spectra of MZI1 and MZI2.</p>
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<p>Schematic diagram of the mode-locked fiber laser based on the Vernier effect filter.</p>
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<p>Characteristics of the dissipative solitons. (<b>a</b>) Spectrum; (<b>b</b>) Pulse train; (<b>c</b>) Autocorrelation trace; (<b>d</b>) RF spectra.</p>
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<p>Characteristics of the three-wavelength switchable pulses. (<b>a</b>) Spectra; (<b>b</b>) Transmission curves of the Vernier effect filter; (<b>c</b>) Autocorrelation traces; (<b>d</b>) RF spectra. The red, blue, and orange curves in (<b>a</b>), (<b>b</b>), and (<b>d</b>) respectively correspond to the spectra, the transmission curve of the filter, and the RF spectra of different wavelengths.</p>
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<p>Spectra scanned repeatedly within one hour when the stretching amount is 0.04 mm.</p>
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<p>Characteristics of the amplifier similaritons. (<b>a</b>) Spectrum; (<b>b</b>) Pulse train; (<b>c</b>) Autocorrelation trace; (<b>d</b>) RF spectra.</p>
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<p>Characteristics of the four-wavelength switchable pulses. (<b>a</b>) Spectra; (<b>b</b>) Transmission curves of the Vernier effect filter; (<b>c</b>) Autocorrelation traces; (<b>d</b>) RF spectra. (<b>e</b>) Dependence of pulse energy on central wavelength. The red, blue, orange, and green curves in (<b>a</b>,<b>b</b>,<b>d</b>) correspond to the spectra, the transmission curve of the filter, and the RF spectra of different wavelengths.</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 378
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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12 pages, 3471 KiB  
Article
Erbium-Doped Tunable Fiber Laser Based on a Vernier Effect Filter
by Yuanzhen Liu, Hailong Xu, Kexin Zhu, Yicun Yao, Yuman Suo and Liqiang Zhang
Photonics 2024, 11(10), 979; https://doi.org/10.3390/photonics11100979 - 18 Oct 2024
Viewed by 437
Abstract
A novel vernier effect filter is designed utilizing two cascaded Mach–Zehnder interferometers (MZIs). Integrating the filter into an erbium-doped fiber laser (EDFL), the tunability of laser wavelength is achieved. Each MZI comprises two sequentially interconnected 3 dB optical couplers (OCs), where the incoming [...] Read more.
A novel vernier effect filter is designed utilizing two cascaded Mach–Zehnder interferometers (MZIs). Integrating the filter into an erbium-doped fiber laser (EDFL), the tunability of laser wavelength is achieved. Each MZI comprises two sequentially interconnected 3 dB optical couplers (OCs), where the incoming light is initially split into two arms at the first OC and subsequently recombined at the second OC. Interference occurs due to the optical path difference between these two beams. Notably, the two MZIs exhibit closely matched free spectral ranges (FSRs), leading to the formation of a broadened envelope in the superimposed spectrum. By delicately adjusting the optical path difference between the two arms of one MZI, a little drift of the interference spectrum is induced. This small amount of drift, in turn, triggers a significant movement of the envelope, giving rise to the so-called vernier effect. Integrating the vernier effect filter into an EDFL, the wavelength of the fiber laser can be tuned from 1542.56 nm to 1556.62 nm, with a tuning range of 14.06 nm. Furthermore, by employing a high-precision stepper motor, a remarkable tuning accuracy of 0.01 nm is attainable. The side mode suppression ratio of all wavelengths is above 55 dB. In comparison to reported tunable fiber lasers utilizing MZI filters, the proposed fiber laser in this study offers enhanced precision and a more user-friendly tuning process. Full article
(This article belongs to the Special Issue Cutting-Edge Developments in Fiber Laser)
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<p>Schematic diagram of the vernier effect filter.</p>
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<p>Transmission curves of MZI1 (<b>a1</b>,<b>b1</b>) and MZI2 (<b>a2</b>,<b>b2</b>), and their superimposed transmission curve (<b>a3</b>,<b>b3</b>) with different FSRs.</p>
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<p>(<b>a</b>) Variation in the peak wavelength of the envelope when the optical path difference of MZI2 is adjusted in increments of 128 nm. (<b>b</b>) Drift in the peak wavelength of the envelope when the optical path difference of MZI2 is adjusted in increments of 8 nm. (<b>c</b>) Variation in the peak wavelength of the envelope when the optical path difference of MZI1 is adjusted in increments of 128 nm.</p>
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<p>(<b>a</b>) Transmission spectrum of MZI2. (<b>b</b>) Transmission spectrum of MZI1. (<b>c</b>) Superimposed spectrum of MZI1 and MZI2. (<b>d</b>) Shift in the superimposed spectrum when one arm of MZI2 is stretched.</p>
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<p>Schematic diagram of the wavelength-tunable EDFL.</p>
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<p>(<b>a</b>) Laser spectra with the increase in pump power. (<b>b</b>) Gain spectra of the Er-doped fiber.</p>
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<p>(<b>a</b>) Spectra of the EDFL with different peak wavelengths. (<b>b</b>) Dependence of the peak wavelength of the EDFL on stretching amount.</p>
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<p>(<b>a</b>) Spectra of the EDFL with a high tuning accuracy of 0.01 nm. (<b>b</b>) Details of the tunable wavelength.</p>
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<p>(<b>a</b>) Dual-wavelength output spectrum at 1542.63 nm and 1544.85 nm. (<b>b</b>) Dual-wavelength output spectrum at 1554.39 nm and 1556.65 nm.</p>
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<p>(<b>a</b>) Wavelength shift during first stretching and retracting of MZI2. (<b>b</b>) Wavelength shift during second stretching and retracting of MZI2.</p>
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<p>(<b>a</b>) Wavelength shifts and power fluctuation in the hour before stretching. (<b>b</b>) Wavelength shifts and power fluctuation in the hour after stretching.</p>
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18 pages, 7980 KiB  
Article
High-Sensitivity Displacement Sensor Using Few-Mode Optical Fibers and the Optical Vernier Effect
by Luis E. Guillen-Ruiz, Gilberto Anzueto-Sánchez, Alejandro Martínez-Rios, Myriam C. Jiménez-Mares and Javier A. Martin-Vela
Appl. Sci. 2024, 14(20), 9300; https://doi.org/10.3390/app14209300 - 12 Oct 2024
Viewed by 786
Abstract
This paper presents a displacement sensor designed to achieve the Optical Vernier Effect (OVE) through a simple yet robust configuration, enhancing sensitivity and precision in small displacement measurements. The sensor structure comprises a few-mode fiber (FMF) placed between two single-mode fibers (SMF) in [...] Read more.
This paper presents a displacement sensor designed to achieve the Optical Vernier Effect (OVE) through a simple yet robust configuration, enhancing sensitivity and precision in small displacement measurements. The sensor structure comprises a few-mode fiber (FMF) placed between two single-mode fibers (SMF) in an SMF-FMF-SMF (SFS) configuration. A series of distinct configurations of concatenated Mach–Zehnder fiber interferometers (MZFI) were examined, with the lengths of the reference FMF (FMFRef) and sensing FMF (FMFSen) adjusted to track the spectral envelope shifts. The results demonstrate that the direction of the spectral shift is governed by the ratio between the FMFRef and FMFSen lengths. The sensor achieved a sensitivity of up to 39.07 nm/mm and a magnification factor (M factor) of up to 50.09, demonstrating exceptional precision and adaptability across a range of applications. The proposed configuration also enhances the overall sensor performance, highlighting its potential for broader use in fields requiring precise displacement monitoring. Full article
(This article belongs to the Special Issue Recent Trends in Fiber Optic Sensor: Technology and Applications)
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<p>Schematic diagram of the cascade MZFIs.</p>
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<p>Transducer made of TPU that correlated the phase difference induced by the curvature of the optical fiber with the linear displacement.</p>
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<p>Experimental setup for the in-cascade MZFIs SFS structure to obtain OVE.</p>
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<p>(<b>a</b>,<b>c</b>) show the transmission spectra of <span class="html-italic">MZFI<sub>Ref</sub></span> and <span class="html-italic">MZFI<sub>Sen</sub></span>, respectively. (<b>b</b>,<b>d</b>) represent their corresponding FFT spectra. (<b>e</b>) is the superimposed transmission of two MZFIs, and (<b>f</b>) is the FFT of the superimposed spectrum.</p>
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<p>(<b>a</b>,<b>c</b>) show the transmission spectra of <span class="html-italic">MZFI<sub>Ref</sub></span> and <span class="html-italic">MZFI<sub>Sen</sub></span>, respectively. (<b>b</b>,<b>d</b>) represent their corresponding FFT spectra. (<b>e</b>) is the superimposed transmission of two MZFIs, and (<b>f</b>) is the FFT of the superimposed spectrum.</p>
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<p>(<b>a</b>,<b>c</b>) show the transmission spectra of <span class="html-italic">MZFI<sub>Ref</sub></span> and <span class="html-italic">MZFI<sub>Sen</sub></span>, respectively. (<b>b</b>,<b>d</b>) represent their corresponding FFT spectra. (<b>e</b>) is the superimposed transmission of two MZFIs, and (<b>f</b>) is the FFT of the superimposed spectrum.</p>
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<p>(<b>a</b>,<b>c</b>) show the transmission spectra of <span class="html-italic">MZFI<sub>Ref</sub></span> and <span class="html-italic">MZFI<sub>Sen</sub></span>, respectively. (<b>b</b>,<b>d</b>) represent their corresponding FFT spectra. (<b>e</b>) is the superimposed transmission of two MZFIs, and (<b>f</b>) is the FFT of the superimposed spectrum.</p>
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<p>(<b>a</b>,<b>c</b>) show the transmission spectra of <span class="html-italic">MZFI<sub>Ref</sub></span> and <span class="html-italic">MZFI<sub>Sen</sub></span>, respectively. (<b>b</b>,<b>d</b>) represent their corresponding FFT spectra. (<b>e</b>) is the superimposed transmission of two MZFIs, and (<b>f</b>) is the FFT of the superimposed spectrum.</p>
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<p>The spectral shift of the envelopes as a function of linear displacement from table 1: (<b>a</b>) experiment 1, (<b>b</b>) experiment 2, (<b>c</b>) experiment 3, (<b>d</b>) experiment 4 and (<b>e</b>) experiment 5.</p>
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<p>Slopes of the envelopes from table 1: (<b>a</b>) experiment 1, (<b>b</b>) experiment 2, (<b>c</b>) experiment 3, (<b>d</b>) experiment 4 and (<b>e</b>) experiment 5.</p>
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<p>Specific characteristics of the first 4 harmonics of the 3 different devices described in table 2: (<b>a</b>) experimental setup 1, (<b>b</b>) experimental setup 2 and (<b>c</b>) experimental setup 3. It is observed that both the peaks and internal envelopes increase in proportion to “<span class="html-italic">i</span> + 1”, where “<span class="html-italic">i</span>” is the harmonic order.</p>
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<p>Spectral shift due to linear displacement. The red arrow indicates the wavelength shift: (<b>a</b>) first harmonic (one intersection); (<b>b</b>) second harmonic (three intersections); (<b>c</b>) third harmonic (six intersections); (<b>d</b>) fourth harmonic (multiple intersections).</p>
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<p>Sensitivity of the first four harmonics of the first device: (<b>a</b>) first harmonic; (<b>b</b>) second harmonic; (<b>c</b>) third harmonic; (<b>d</b>) fourth harmonic.</p>
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<p>Five devices demonstrating Blueshift (red arrows) in panels (<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>,<b>i</b>) and Redshift (blue arrows) in panels (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>,<b>j</b>).</p>
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11 pages, 5235 KiB  
Article
High-Sensitivity Refractive Index Sensing Based on an SNPNS Composite Structure
by Di Wu, Jingwen Zhou, Xiang Yu and Yue Sun
Photonics 2024, 11(10), 941; https://doi.org/10.3390/photonics11100941 - 7 Oct 2024
Viewed by 516
Abstract
In this paper, we design and demonstrate an all-fiber-sensitive refractive index (RI) sensor based on the Mach–Zehnder interferometer (MZI). It is constructed by splicing two no-core fibers (NCFs) and a photonic crystal fiber (PCF) between two single-mode fibers (SMFs) to obtain an SMF–NCF–PCF–NCF–SMF [...] Read more.
In this paper, we design and demonstrate an all-fiber-sensitive refractive index (RI) sensor based on the Mach–Zehnder interferometer (MZI). It is constructed by splicing two no-core fibers (NCFs) and a photonic crystal fiber (PCF) between two single-mode fibers (SMFs) to obtain an SMF–NCF–PCF–NCF–SMF composite structure (SNPNS). A study of the effect of varying PCF lengths on the RI reveals that the shorter the length, the higher the sensitivity. The maximum RI sensitivity of 176.9 nm/RIU is attained within the RI range of 1.3365–1.3767 when the PCF length in the SNPNS structure is 3 cm. Meanwhile, the sensor exhibits a high stability in water, with an RSD of only 0.0019% for the interference trough over a duration of two hours. This proposed sensing structure offers the advantages of a large extinction ratio, small size, low temperature sensitivity, and simple fabrication, exhibiting a great potential in RI measurements. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
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<p>Schematic diagram of the MZI sensor based on the SNPNS composite structure.</p>
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<p>Cross-section of PCF under the electron microscope.</p>
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<p>Simulated field distributions of SNPNS composite structure with lengths of NCF<sub>1</sub>, PCF, and NCF<sub>2</sub> equal to 3 cm.</p>
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<p>Diagram of the experimental setup.</p>
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<p>Transmission spectra of SNPNS composite structure sensors for PCF lengths of 3 cm, 4 cm, and 5 cm.</p>
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<p>Spatial spectra of SNPNS composite structure sensors for PCF lengths of 3 cm, 4 cm, and 5 cm.</p>
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<p>The SNPNS composite structure sensor with PCF length of 3 cm and (<b>a</b>–<b>c</b>) transmission spectra responses for dips A, B, and C with different RI values; (<b>d</b>) relationships between interference dips and RI values.</p>
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<p>The SNPNS composite structure sensor with PCF length of 4 cm and (<b>a</b>) transmission spectra responses with different RI values and (<b>b</b>) relationships between interference dips and RI values.</p>
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<p>The SNPNS composite structure sensor with PCF length of 5 cm and (<b>a</b>) transmission spectra response with different RI values and (<b>b</b>) relationships between interference dips and RI values.</p>
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<p>(<b>a</b>) Transmission spectrum of the sensor with PCF length of 3 cm in water; (<b>b</b>) stability lines of different dips at the water temperature of 23 °C; (<b>c</b>) relationships between interference dips and water temperature.</p>
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12 pages, 6463 KiB  
Communication
Balloon-Shaped SMF Blood Glucose Concentration and Temperature Sensor Based on Core-Offset Structure
by Weihua Zhang, Yixi Liu, Zhengrong Tong, Xue Wang, Yipeng Tao, Haozheng Yu and Jinlin Mu
Sensors 2024, 24(19), 6344; https://doi.org/10.3390/s24196344 - 30 Sep 2024
Viewed by 415
Abstract
A blood glucose concentration and temperature sensor with a balloon-shaped single-mode fiber (SMF) based on a core-offset structure is proposed and experimentally demonstrated. The balloon-shaped SMF is created by offset-fusing a straight-line SMF between two other SMFs, thereby forming a Mach–Zehnder interferometer (MZI). [...] Read more.
A blood glucose concentration and temperature sensor with a balloon-shaped single-mode fiber (SMF) based on a core-offset structure is proposed and experimentally demonstrated. The balloon-shaped SMF is created by offset-fusing a straight-line SMF between two other SMFs, thereby forming a Mach–Zehnder interferometer (MZI). The core-offset structure can effectively excite higher-order cladding modes. The experimental results showed that the maximum sensitivity of blood glucose concentration was 0.331 nm/(mmol/l) and the maximum sensitivity of temperature was 0.216 nm/°C when the offset distance was 10 μm. Dual-parameter measurement was achieved through a dual-parameter matrix. In addition, the sensor has characteristics such as simple structure, low cost, good stability, and electromagnetic interference resistance, making it potentially valuable for diagnosing high blood glucose and related conditions. Full article
(This article belongs to the Section Biomedical Sensors)
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<p>(<b>a</b>) The schematic diagram of the proposed sensor. (<b>b</b>) The physical diagram of the proposed sensor.</p>
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<p>The fabrication process of the balloon-shaped SMF based on the core-offset structure. (<b>a</b>) First staggered-core structural fabrication. (<b>b</b>) Second staggered-core structure fabrication. (<b>c</b>) Fabrication of balloon structure.</p>
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<p>Refractive index distribution of SMF.</p>
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<p>The energy field distribution diagram and normalized energy diagram of l = 10 μm.</p>
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<p>Experimental sensing device.</p>
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<p>Spatial spectrum diagram of l = 10 μm.</p>
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<p>Blood glucose concentration experimental results of sensor 1. (<b>a</b>) Spectrogram of the blood glucose concentration experiment of sensor 1. (<b>b</b>) Experimental linear fit of blood glucose concentration for Sensor 1.</p>
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<p>Blood glucose concentration experimental results of sensor 2. (<b>a</b>) Spectrogram of the blood glucose concentration experiment of sensor 2. (<b>b</b>) Experimental linear fit of blood glucose concentration for Sensor 2.</p>
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<p>Blood glucose concentration experimental results of sensor 3. (<b>a</b>) Spectrogram of the blood glucose concentration experiment of sensor 3. (<b>b</b>) Experimental linear fit of blood glucose concentration for Sensor 3.</p>
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<p>Experimental comparison of blood glucose concentration with different offset sensors.</p>
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<p>Temperature experimental results of sensor 1. (<b>a</b>) Spectrogram of the temperature experiment of sensor 1. (<b>b</b>) Experimental linear fit of temperature for Sensor 1.</p>
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<p>Temperature experimental results of sensor 2. (<b>a</b>) Spectrogram of the temperature experiment of sensor 2. (<b>b</b>) Experimental linear fit of temperature for Sensor 2.</p>
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<p>Temperature experimental results of sensor 3. (<b>a</b>) Spectrogram of the temperature experiment of sensor 3. (<b>b</b>) Experimental linear fit of temperature for Sensor 3.</p>
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<p>Experimental comparison of temperature with different offset sensors.</p>
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<p>(<b>a</b>) Blood glucose concentration stability experiment results. (<b>b</b>) Temperature stability experiment results.</p>
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16 pages, 5561 KiB  
Article
A Hybrid GAN-Inception Deep Learning Approach for Enhanced Coordinate-Based Acoustic Emission Source Localization
by Xuhui Huang, Ming Han and Yiming Deng
Appl. Sci. 2024, 14(19), 8811; https://doi.org/10.3390/app14198811 - 30 Sep 2024
Viewed by 914
Abstract
In this paper, we propose a novel approach to coordinate-based acoustic emission (AE) source localization to address the challenges of limited and imbalanced datasets from fiber-optic AE sensors used for structural health monitoring (SHM). We have developed a hybrid deep learning model combining [...] Read more.
In this paper, we propose a novel approach to coordinate-based acoustic emission (AE) source localization to address the challenges of limited and imbalanced datasets from fiber-optic AE sensors used for structural health monitoring (SHM). We have developed a hybrid deep learning model combining four generative adversarial network (GAN) variants for data augmentation with an adapted inception neural network for regression-based prediction. The experimental setup features a single fiber-optic AE sensor based on a tightly coiled fiber-optic Fabry-Perot interferometer formed by two identical fiber Bragg gratings. AE signals were generated using the Hsu-Nielsen pencil lead break test on a grid-marked thin aluminum plate with 35 distinct locations, simulating real-world structural monitoring conditions in bounded isotropic plate-like structures. It is demonstrated that the single-sensor configuration can achieve precise localization, avoiding the need for a multiple sensor array. The GAN-based signal augmentation expanded the dataset from 900 to 4500 samples, with the Wasserstein distance between the original and synthetic datasets decreasing by 83% after 2000 training epochs, demonstrating the high fidelity of the synthetic data. Among the GAN variants, the standard GAN architecture proved the most effective, outperforming other variants in this specific application. The hybrid model exhibits superior performance compared to non-augmented deep learning approaches, with the median error distribution comparisons revealing a significant 50% reduction in prediction errors, accompanied by substantially improved consistency across various AE source locations. Overall, this developed hybrid approach offers a promising solution for enhancing AE-based SHM in complex infrastructures, improving damage detection accuracy and reliability for more efficient predictive maintenance strategies. Full article
(This article belongs to the Special Issue Advanced Optical-Fiber-Related Technologies)
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<p>Schematic of the fiber-optic coil-based acoustic emission sensing system. Inset: Close-up image of the sensor, showing the flexible mounting and dimensions (8 mm outer, 6 mm inner diameter).</p>
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<p>(<b>a</b>) Aluminum plate with the grid and fiber-optic sensor for AE testing (<b>b</b>) Schematic representation of the aluminum plate detailing the grid layout and test points.</p>
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<p>Time series augmentation showing the original data (orange) and generated data (green) to ensure each label has a balanced and sufficient number of samples for improved deep learning model performance.</p>
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<p>(<b>a</b>) Workflow of the hybrid network for AE source localization (<b>b</b>) Architecture of the Inception network for regression.</p>
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<p>Architecture of the generator and discriminator networks in the GAN for AE signal augmentation.</p>
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<p>The t-SNE visualization of synthetic and original datasets (<b>a</b>) The training epoch of 1 for GAN (<b>b</b>) The training epoch of 2000 for GAN (<b>c</b>) The training epoch of 2000 for WGAN (<b>d</b>) The training epoch of 2000 for DCGAN (<b>e</b>) The training epoch of 2000 for TSAGAN (<b>f</b>) Augmentation via addition of noise.</p>
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<p>The comparison of Wasserstein distance convergence across epochs for the four GAN variants (GAN, TSAGAN, WGAN, and DCGAN).</p>
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<p>The comparison of acoustic emission (AE) source localization performance. (<b>a</b>) Results from the hybrid deep learning model with GAN-based data augmentation and Inception network. (<b>b</b>) Results from the Inception network alone without GAN-based augmentation. Square markers represent actual source locations, star markers show predicted locations, and the large circular marker indicates the sensor position. The x and y axes represent dimensions in inches.</p>
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<p>The comparison of errors for the different methods.</p>
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12 pages, 3631 KiB  
Article
Fiber Bragg Grating Pulse and Systolic Blood Pressure Measurement System Based on Mach–Zehnder Interferometer
by Yuanjun Li, Bo Wang, Shanren Liu, Mengmeng Gao, Qianhua Li, Chao Chen, Qi Guo and Yongsen Yu
Sensors 2024, 24(19), 6222; https://doi.org/10.3390/s24196222 - 26 Sep 2024
Viewed by 506
Abstract
A fiber Bragg grating (FBG) pulse and systolic blood pressure (SBP) measurement system based on the edge-filtering method is proposed. The edge filter is the Mach–Zehnder interferometer (MZI) fabricated by two fiber couplers with a linear slope of 52.45 dBm/nm. The developed system [...] Read more.
A fiber Bragg grating (FBG) pulse and systolic blood pressure (SBP) measurement system based on the edge-filtering method is proposed. The edge filter is the Mach–Zehnder interferometer (MZI) fabricated by two fiber couplers with a linear slope of 52.45 dBm/nm. The developed system consists of a broadband light source, an edge filter, fiber Bragg gratings (FBGs), a coarse wavelength-division multiplexer (CWDM), and signal-processing circuits based on a field-programmable gate array (FPGA). It can simultaneously measure pulse pulsations of the radial artery in the wrist at three positions: Cun, Guan and Chi. The SBP can be calculated based on the pulse transit time (PTT) principle. The measurement results compared to a standard blood pressure monitor showed the mean absolute error (MAE) and standard deviation (STD) of the SBP were 0.93 ± 3.13 mmHg. The system meets the requirements of the Association for the Advancement of Medical Instrumentation (AAMI) equipment standards. The proposed system can achieve continuous real-time measurement of pulse and SBP and has the advantages of fast detection speed, stable performance, and no compression sensation for subjects. The system has important application value in the fields of human health monitoring and medical device development. Full article
(This article belongs to the Section Optical Sensors)
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<p>Schematic diagram of pulse and systolic blood pressure (SBP) measurement system. (<b>a</b>) Schematic diagram of pulse measurement; (<b>b</b>) Schematic diagram of SBP measurement.</p>
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<p>(<b>a</b>) Interference spectra of the Mach–Zehnder interferometers with varying arm length differences; (<b>b</b>) interference spectrum of the Mach–Zehnder interferometer (MZI) with arm length difference of 2 mm; (<b>c</b>) spatial frequency spectrum of the MZI with arm length differences of 2 mm; (<b>d</b>) linearity of the MZI in the range of 1589.45–1589.70 nm.</p>
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<p>Principle and physical diagram of the photoelectric amplifier circuit and a field-programmable gate array (FPGA) module.</p>
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<p>(<b>a</b>) Distribution diagram of fiber Bragg gratings (FBGs); (<b>b</b>) reflection spectra of FBGs.</p>
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<p>Pulse waveforms measured by the cascaded FBGs at the positions of Cun, Guan, and Chi.</p>
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<p>The pulse waveform of a single cycle collected by the system. (A: Starting point of pulse wave; B: Crest; C: Tidal wave; D: Dicrotic notch; E: Dicrotic wave; F: End point of pulse wave).</p>
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<p>(<b>a</b>) Radial artery waveforms of left and right hands of subjects; (<b>b</b>) relationship between SBP and ln (1/PTT).</p>
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<p>(<b>a</b>) Bland-Altman plot of measured and reference values of SBP; (<b>b</b>) relationship between measured SBP and reference values.</p>
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10 pages, 5697 KiB  
Article
Ultrahigh Extinction Ratio Leaky-Guided Hollow Core Fiber Mach–Zehnder Interferometer Assisted by a Large Core Hollow Fiber Beam Splitter
by Yan-Han Lu, Ren-Xiang Luo and Cheng-Ling Lee
Nanomaterials 2024, 14(18), 1494; https://doi.org/10.3390/nano14181494 - 14 Sep 2024
Viewed by 630
Abstract
We proposed a novel fiber Mach–Zehnder interferometer (FMZI) that can perform an ultrahigh extinction ratio (ER), ultracompact, and ultra-broadband interference characteristics. The FMZI structure is based on an extremely tiny hollow core fiber (HCF) with a small diameter of 10 μm (named HCF [...] Read more.
We proposed a novel fiber Mach–Zehnder interferometer (FMZI) that can perform an ultrahigh extinction ratio (ER), ultracompact, and ultra-broadband interference characteristics. The FMZI structure is based on an extremely tiny hollow core fiber (HCF) with a small diameter of 10 μm (named HCF10) connected with a beam splitter of a large core of 50 μm HCF (named HCF50). The refractive index (RI) of the air core is lower than that of the HCF cladding; a leaky-guided fiber waveguide (LGFW) occurs in such a short-section HCF10 waveguide to simultaneously have the core and cladding modes. To achieve better fringe visibility of the interference, the section of HCF50 assists in splitting the optical light into core and cladding beams launched into the HCF10 with appropriate intensities. Experimental and simulation results show that the optical characteristics of the proposed LGFW-FMZI are very similar. Based on the results of the study, the length of the HCF10 primarily influences the free spectral range (FSR) of the interference spectra, and the HCF50 splitter significantly controls the optimal extinction ratio (ER) of the interference fringes. By exactly adjusting the lengths of HCF10 and HCF50, the proposed fiber interferometers can perform the capability of an ultrahigh ER over 50 dB with the arbitrary FSR in the transmitted interference spectra over an ultra-broad wavelength range of 1250 nm to 1650 nm. Full article
(This article belongs to the Section Nanophotonics Materials and Devices)
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<p>(<b>a</b>) Schematic diagram of the proposed HCF-based LGFW-FMZI. The FDBPM simulation results of optical field distribution of light for the proposed structure (<b>b</b>) with and (<b>c</b>) without the segment of the HCF<sub>50</sub> beam splitter.</p>
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<p>Simulated interference spectra for different combinations of L<sub>50</sub> and L<sub>10</sub> in the proposed leaky-guided FMZI with varying L<sub>50</sub> from 50 to 140 μm and fixed L<sub>10</sub> are (<b>a</b>) 30 μm, (<b>b</b>) 55 μm, (<b>c</b>) 95 μm, and (<b>d</b>) 140 μm, respectively.</p>
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<p>Simulation results for the best ultrahigh ER around 50 dB of the optimal interferences at L<sub>10</sub> fixed at (<b>a</b>) 30 μm, (<b>b</b>) 55 μm, (<b>c</b>) 95 μm, and (<b>d</b>) 140 μm when the L<sub>50</sub> is 89.4 μm, 84.4 μm, 82.2 μm, and 70.8 μm, respectively. (Note: the monitored wavelength range is 1460 nm–1625 nm).</p>
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<p>The FSR of the proposed leaky-guided FMZI with varying L<sub>50</sub> of HCF<sub>50</sub> when the L<sub>10</sub> of HCF<sub>10</sub> is fixed at (<span class="html-fig-inline" id="nanomaterials-14-01494-i001"><img alt="Nanomaterials 14 01494 i001" src="/nanomaterials/nanomaterials-14-01494/article_deploy/html/images/nanomaterials-14-01494-i001.png"/></span>) 30 μm, (<span class="html-fig-inline" id="nanomaterials-14-01494-i002"><img alt="Nanomaterials 14 01494 i002" src="/nanomaterials/nanomaterials-14-01494/article_deploy/html/images/nanomaterials-14-01494-i002.png"/></span>) 55 μm, (<span class="html-fig-inline" id="nanomaterials-14-01494-i003"><img alt="Nanomaterials 14 01494 i003" src="/nanomaterials/nanomaterials-14-01494/article_deploy/html/images/nanomaterials-14-01494-i003.png"/></span>) 95 μm, and (<span class="html-fig-inline" id="nanomaterials-14-01494-i004"><img alt="Nanomaterials 14 01494 i004" src="/nanomaterials/nanomaterials-14-01494/article_deploy/html/images/nanomaterials-14-01494-i004.png"/></span>) 140 μm, respectively.</p>
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<p>The ERs of interference fringe around λ = 1550 nm in the proposed leaky-guided FMZI with varying L<sub>50</sub> of HCF<sub>50</sub> when the L<sub>10</sub> of HCF<sub>10</sub> is fixed.</p>
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<p>Schematic diagrams of (<b>a</b>) the fabrication steps and (<b>b</b>) the measurement system.</p>
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<p>Comparison of the optical interference spectra of the simulation (optimal) and experimental results with fabricated L<sub>50</sub>/L<sub>10</sub> (<b>a</b>) 90.5/28.8 μm, (<b>b</b>) 86.7/55.9 μm, (<b>c</b>) 81.5/96.6 μm, and (<b>d</b>) 72.5/140 μm, respectively. Their insets include a corresponding microscopic image of the fabricated devices.</p>
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10 pages, 3674 KiB  
Article
An S-Shaped Core M-Z Interferometer Induced by Arc-Discharging for Strain Sensing
by Xiaoyang Li, Jiarui Chen, Shengjia Wang, Yongjun Liu and Tao Geng
Photonics 2024, 11(9), 816; https://doi.org/10.3390/photonics11090816 - 30 Aug 2024
Viewed by 841
Abstract
In this study, a kind of in-fiber Mach–Zehnder interferometer (MZI) is designed and experimentally examined. The MZI is composed of two in-fiber S-shaped cores (SSCs), which enhance strain sensitivity. To prepare the SSCs, a high-frequency CO2 laser is first utilized to polish [...] Read more.
In this study, a kind of in-fiber Mach–Zehnder interferometer (MZI) is designed and experimentally examined. The MZI is composed of two in-fiber S-shaped cores (SSCs), which enhance strain sensitivity. To prepare the SSCs, a high-frequency CO2 laser is first utilized to polish grooves on the symmetrical surface of a single-mode fiber (SMF). The polished area is then subjected to arc-discharging by a commercial fusion splicer, and the core of the fiber bends towards the polished grooves due to the self-roundness of the cladding and the heating effect of discharge. The results of the experiments demonstrate that the sensor achieves high strain sensitivities of −66.5 pm/με and −40.1 pm/με within the strain range of 0 με to 350 με. By solving the matrix equation, simultaneous online measurements of temperature and strain can be performed. With the advantages of easy fabrication, low cost, high sensitivity, and compactness, the proposed sensor is a competitive candidate in strain sensing. Full article
(This article belongs to the Special Issue Advances in Optical Fiber Sensing Technology)
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<p>Schematic diagram of SSC−MZI.</p>
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<p>Simulation results of light energy distribution of (<b>a</b>) SSC−MZI and (<b>b</b>) structure with smaller parameters.</p>
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<p>Evolution of simulated spectrum of SSC−MZI with increasing interference length.</p>
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<p>Schematic diagram of CO<sub>2</sub> laser polishing and arc-discharging.</p>
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<p>Side view of (<b>a</b>) polished structure. (<b>b</b>) Arc−discharged structure. (<b>c</b>) Transmission spectrum of proposed SSC−MZI.</p>
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<p>The spectral comparison of three SSC−MZIs with identical parameters.</p>
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<p>Spectrum responses to strain of (<b>a</b>) Dip A and (<b>b</b>) Dip B. Linear fitting result for wavelength and strain of (<b>c</b>) Dip A and (<b>d</b>) Dip B.</p>
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<p>Spectrum responses of temperature of (<b>a</b>) Dip A and (<b>b</b>) Dip B. Linear fitting result for wavelength and temperature of (<b>c</b>) Dip A and (<b>d</b>) Dip B.</p>
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<p>The comparison between actual and experimental values of temperature and strain.</p>
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14 pages, 3988 KiB  
Article
Study on the Detection of Single and Dual Partial Discharge Sources in Transformers Using Fiber-Optic Ultrasonic Sensors
by Feng Liu, Yansheng Shi, Shuainan Zhang and Wei Wang
Photonics 2024, 11(9), 815; https://doi.org/10.3390/photonics11090815 - 29 Aug 2024
Viewed by 3198
Abstract
Partial discharge is a fault that occurs at the site of insulation defects within a transformer. Dual instances of partial discharge origination discharging simultaneously embody a more intricate form of discharge, where the interaction between the discharge sources leads to more intricate and [...] Read more.
Partial discharge is a fault that occurs at the site of insulation defects within a transformer. Dual instances of partial discharge origination discharging simultaneously embody a more intricate form of discharge, where the interaction between the discharge sources leads to more intricate and unpredictable insulation damage. Conventional piezoelectric transducers are magnetically affixed to the exterior metal tank of transformers. The ultrasonic signals emanating from partial discharge undergo deflection and reverberation upon traversing the windings, insulation paperboards, and the outer shell, resulting in signal attenuation and thus making it difficult to detect such faults. Furthermore, it is challenging to distinguish between simultaneous discharges from dual partial discharge sources and continuous discharges from a single source, often leading to missed detection and repairs of fault points, which increase the maintenance difficulty and cost of power equipment. With the advancement of MEMS (Micro-Electro-Mechanical System) technology, fiber-optic ultrasonic sensors have surfaced as an innovative technique for optically detecting partial discharges. These sensors are distinguished by their minute dimensions, heightened sensitivity, and robust immunity to electromagnetic disturbances. and excellent insulation properties, allowing for internal installation within power equipment for partial discharge monitoring. In this study, we developed an EFPI (Extrinsic Fabry Perot Interferometer) optical fiber ultrasonic sensor that can be installed inside transformers. Based on this sensor array, we also created a partial discharge ultrasonic detection system that estimates the directional information of single and dual partial discharge sources using the received signals from the sensor array. By utilizing the DOA (Direction of Arrival) as a feature recognition parameter, our system can effectively detect both simultaneous discharges from dual partial discharge sources and continuous discharges from a single source within transformer oil tanks, meeting practical application requirements. The detection methodology presented in this paper introduces an original strategy and resolution for pinpointing the types of partial discharges occurring under intricate conditions within power apparatus, effectively distinguishing between discharges from single and dual partial discharge sources. Full article
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<p>Configuration of the EFPI sensor.</p>
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<p>Structure of EFPI fiber-optic ultrasonic sensor manufacturing system.</p>
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<p>Physical diagram of the hardware platform.</p>
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<p>Dual PD signals measured by fiber-optic ultrasonic sensor.</p>
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<p>The diagrammatic depiction of the square array element structure (<b>a</b>) Plan view; (<b>b</b>) Space arrangement diagram.</p>
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<p>The diagrammatic depiction of the regular tetrahedron array element structure (<b>a</b>) Plan view; (<b>b</b>) Space arrangement diagram.</p>
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<p>DOA Estimation Diagram.</p>
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<p>Simulation waveform of partial discharge.</p>
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<p>Directional measurement layout diagrams of different array models (<b>a</b>) Square array; (<b>b</b>) Regular tetrahedral array.</p>
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<p>Test setup of direction finding experiment for dual PD sources.</p>
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<p>Test setup of direction finding experiment for continuous discharge of single PD source.</p>
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<p>The Signal of two consecutive discharges from a single PD source captured by sensor.</p>
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