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11 pages, 18207 KiB  
Article
Manufacturing Anti-Reflective Subwavelength Structures on ZnS Using Femtosecond Laser Bessel Beam with Burst Mode
by Haoran Wang, Biwen Li, Liangbin Hu and Fan Zhang
Biomimetics 2024, 9(11), 655; https://doi.org/10.3390/biomimetics9110655 - 26 Oct 2024
Viewed by 447
Abstract
Increasing the transmittance of zinc sulfide (ZnS) infrared windows can effectively improve the imaging quality of infrared detection. In this study, an anti-reflective subwavelength structure (ASS) was manufactured on ZnS using a femtosecond burst Bessel laser with the goal of achieving high transmittance [...] Read more.
Increasing the transmittance of zinc sulfide (ZnS) infrared windows can effectively improve the imaging quality of infrared detection. In this study, an anti-reflective subwavelength structure (ASS) was manufactured on ZnS using a femtosecond burst Bessel laser with the goal of achieving high transmittance in the mid-infrared range. The period and depth parameters of the ASS were initially determined using the effective medium approximation (EMA) theory and subsequently optimized using the rigorous coupled-wave analysis (RCWA) method to eliminate surface Fresnel anti-reflections. The depth of the ASS increases with the number of bursts, while the structure profile transitions from Gaussian to conical. In addition, the ASS achieves 86% transmittance in the 7–10 µm range, and the average transmittance improves by 10% in the 5–12 µm range. Moreover, the wide-angle ASS with the hydrophobicity (contact angle 160°) is achieved on the ZnS window. Ultimately, the ASS on ZnS enhances the clarity of the infrared image. Full article
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<p>(<b>a</b>) Photograph of cicada wings and SEM image of transparent anti-reflective area; (<b>b</b>,<b>c</b>) schematic diagram of femtosecond burst Bessel processing system (modes consisting of N = 1, 2, 4, and 8 pulses with t<sub>sep</sub> = 25 ns); (<b>d</b>) schematic diagram of manufacturing process of conical array zinc sulfide anti-reflective surface; (<b>e</b>) image of ZnS anti-reflective surface under light.</p>
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<p>(<b>a</b>,<b>b</b>) The simulated electric field strength distribution at an incident wavelength of 10 μm for ASS periods of 2.5 μm and 3.0 μm; (<b>c</b>) a contour plot of the simulated ASS transmittance versus the incident wavelength, λ, and period, p; (<b>d</b>) the simulated transmission spectra of the ASS for wavelengths ranging from 2.5 to 13.5 μm.</p>
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<p>(<b>a</b>,<b>b</b>) The simulated electric field strength distribution at an incident wavelength of 10 μm for ASS depths of 1.5 μm and 2.5 μm; (<b>c</b>) a contour plot of simulated ASS transmittance versus the incident wavelength, λ, and depth, h; (<b>d</b>) the simulated transmission spectra of the ASS for wavelengths ranging from 2.5 to 13.5 μm.</p>
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<p>The SEM of the ASS with 6 μJ pulse energy: (<b>a</b>,<b>b</b>) burst 8; (<b>c</b>) burst 1. (<b>d</b>) The diameters for different parameters of the ASS.</p>
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<p>The profiles of the ASS with 6 μJ pulse energy and (<b>a</b>) burst 8, (<b>b</b>) burst 2, and (<b>c</b>) burst 1 mode; (<b>d</b>) the profiles of the ASS with different pulse energies and burst modes.</p>
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<p>(<b>a</b>) Simulated and experimental infrared transmittance of flat ZnS and ASS. Infrared transmittance spectra in (<b>b</b>) different burst modes, (<b>c</b>) different pulse energies, and (<b>d</b>) different incident angles.</p>
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<p>(<b>a</b>) A hydrophobic image of the ASS fabricated on the surface of zinc sulfide; (<b>b</b>) the wettability of the ASS; infrared thermogram images of flat ZnS (<b>c</b>) and ASS (<b>d</b>). The white scale bar represents 5 mm.</p>
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19 pages, 2448 KiB  
Article
MM-IRSTD: Conv Self-Attention-Based Multi-Modal Small and Dim Target Detection in Infrared Dual-Band Images
by Junyan Yang, Zhihui Ye, Jian Lin, Dongfang Chen, Lingbian Du and Shaoyi Li
Remote Sens. 2024, 16(21), 3937; https://doi.org/10.3390/rs16213937 - 23 Oct 2024
Viewed by 612
Abstract
Infrared multi-band small and dim target detection is an important research direction in the fields of modern remote sensing and military surveillance. However, achieving high-precision detection remains challenging due to the small scale, low contrast of small and dim targets, and their susceptibility [...] Read more.
Infrared multi-band small and dim target detection is an important research direction in the fields of modern remote sensing and military surveillance. However, achieving high-precision detection remains challenging due to the small scale, low contrast of small and dim targets, and their susceptibility to complex background interference. This paper innovatively proposes a dual-band infrared small and dim target detection method (MM-IRSTD). In this framework, we integrate a convolutional self-attention mechanism module and a self-distillation mechanism to achieve end-to-end dual-band infrared small and dim target detection. The Conv-Based Self-Attention module consists of a convolutional self-attention mechanism and a multilayer perceptron, effectively extracting and integrating input features, thereby enhancing the performance and expressive capability of the model. Additionally, this module incorporates a dynamic weight mechanism to achieve adaptive feature fusion, significantly reducing computational complexity and enhancing the model’s global perception capability. During model training, we use a spatial and channel similarity self-distillation mechanism to drive model updates, addressing the similarity discrepancy between long-wave and mid-wave image features extracted through deep learning, thus improving the model’s performance and generalization capability. Furthermore, to better learn and detect edge features in images, this paper designs an edge extraction method based on Sobel. Finally, comparative experiments and ablation studies validate the advancement and effectiveness of our proposed method. Full article
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<p>MM-IRSTD structure.</p>
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<p>Conv-based self-attention module schematic.</p>
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<p>Schematic of the Sobel operator.</p>
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<p>Geometric transfer loss from <math display="inline"><semantics> <mrow> <msub> <mi>l</mi> <mi>i</mi> </msub> </mrow> </semantics></math> to <math display="inline"><semantics> <mrow> <msub> <mi>m</mi> <mi>i</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Sample of the dataset. The red box contains the target, and the blue box shows the enlarged view of the target.</p>
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<p>The variation of training loss and testing loss with epochs.</p>
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<p>Qualitative analysis of results. Mid-wave represents the mid-wave image, while Long-wave represents the long-wave image. The red box indicates the target, and the blue box shows the situation after the target has been magnified.</p>
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<p>Incorrect detection examples. In the detection results, the green box indicates correctly detected targets, while the red box indicates incorrectly detected targets. In the labeled original images, the area within the green edges represents the target.</p>
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13 pages, 4137 KiB  
Article
Research on Through-Flame Imaging Using Mid-Wave Infrared Camera Based on Flame Filter
by Fengxun Zheng, Guodong Sun, Yanpeng Suo, Hao Ma and Tengxiao Feng
Sensors 2024, 24(20), 6696; https://doi.org/10.3390/s24206696 - 18 Oct 2024
Viewed by 537
Abstract
High-temperature furnaces and coal-fired boilers are widely employed in the petrochemical and metal-smelting sectors. Over time, the deterioration, corrosion, and wear of pipelines can lead to equipment malfunctions and safety incidents. Nevertheless, effective real-time monitoring of equipment conditions remains insufficient, primarily due to [...] Read more.
High-temperature furnaces and coal-fired boilers are widely employed in the petrochemical and metal-smelting sectors. Over time, the deterioration, corrosion, and wear of pipelines can lead to equipment malfunctions and safety incidents. Nevertheless, effective real-time monitoring of equipment conditions remains insufficient, primarily due to the interference caused by flames generated from fuel combustion. To address this issue, in this study, a through-flame infrared imager is developed based on the mid-wave infrared (MWIR) radiation characteristics of the flame. The imager incorporates a narrowband filter that operates within the wavelength range of 3.80 μm to 4.05 μm, which is integrated into conventional thermal imagers to perform flame filtering. This configuration enables the radiation from the background to pass through the flame and reach the detector, thereby allowing the infrared imager to visualize objects obscured by the flame and measure their temperatures directly. Our experimental findings indicate that the imager is capable of through-flame imaging; specifically, when the temperature of the target exceeds 50 °C, the imager can effectively penetrate the outer flame of an alcohol lamp and distinctly capture the target’s outline. Importantly, as the temperature of the target increases, the clarity of the target’s contour in the images improves. The MWIR through-flame imager presents considerable potential for the real-time monitoring and preventive maintenance of high-temperature furnaces and similar equipment, such as detecting the degradation of refractory materials and damage to pipelines. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>(<b>a</b>) Infrared emission spectrum of a Bunsen burner flame [<a href="#B23-sensors-24-06696" class="html-bibr">23</a>]; (<b>b</b>) transmittance of CO<sub>2</sub>, CO, and H<sub>2</sub>O gasses.</p>
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<p>A schematic diagram of MWIR through-flame imaging.</p>
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<p>The transmittance curve of the flame filter.</p>
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<p>The FG390 camera (<b>a</b>) and its infrared image with temperature measurement (<b>b</b>).</p>
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<p>The experimental composition of MWIR through-flame imaging.</p>
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<p>A 3D view of the alcohol lamp flame.</p>
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<p>The visible-light images (<b>a</b>–<b>f</b>) and infrared images (<b>g</b>–<b>l</b>) at different target temperatures of 20 °C to 300 °C.</p>
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<p>Comparison of wide-band infrared image (<b>a</b>) and through-flame image (<b>b</b>).</p>
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<p>Six 3D views at different temperature levels, illustrating the variations in the raw data (digital number value) across the 80 × 80 pixel area of the alcohol lamp’s outer flame and the target.</p>
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<p>Curve of target–flame ratio (TFR) versus target temperature.</p>
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<p>A visible-light image (<b>a</b>) and an infrared image (<b>b</b>) of pipelines in a tube furnace captured by the through-flame imager.</p>
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20 pages, 10612 KiB  
Review
Review of Photodetectors for Space Lidars
by Xiaoli Sun
Sensors 2024, 24(20), 6620; https://doi.org/10.3390/s24206620 - 14 Oct 2024
Viewed by 493
Abstract
Photodetectors play a critical role in space lidars designed for scientific investigations from orbit around planetary bodies. The detectors must be highly sensitive due to the long range of measurements and tight constraints on the size, weight, and power of the instrument. The [...] Read more.
Photodetectors play a critical role in space lidars designed for scientific investigations from orbit around planetary bodies. The detectors must be highly sensitive due to the long range of measurements and tight constraints on the size, weight, and power of the instrument. The detectors must also be space radiation tolerant over multi-year mission lifetimes with no significant performance degradation. Early space lidars used diode-pumped Nd:YAG lasers with a single beam for range and atmospheric backscattering measurements at 1064 nm or its frequency harmonics. The photodetectors used were single-element photomultiplier tubes and infrared performance-enhanced silicon avalanche photodiodes. Space lidars have advanced to multiple beams for surface topographic mapping and active infrared spectroscopic measurements of atmospheric species and surface composition, which demand increased performance and new capabilities for lidar detectors. Higher sensitivity detectors are required so that multi-beam and multi-wavelength measurements can be performed without increasing the laser and instrument power. Pixelated photodetectors are needed so that a single detector assembly can be used for simultaneous multi-channel measurements. Photon-counting photodetectors are needed for active spectroscopy measurements from short-wave infrared to mid-wave infrared. HgCdTe avalanche photodiode arrays have emerged recently as a promising technology to fill these needs. This paper gives a review of the photodetectors used in past and present lidars and the development and outlook of HgCdTe APD arrays for future space lidars. Full article
(This article belongs to the Section Remote Sensors)
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<p>Photographs of the PMT used in ICESat-2/ATLAS. They were made by Hamamatsu Corporation, Model R7600-300-M16, and up-screened and space-qualified at NASA. The PMT consists of an extended bi-alkali photocathode, a 10-stage dynode chain, and 4 × 4 segmented anodes. There are 16 outputs, one for each anode.</p>
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<p>Photographs and micrographs of the silicon APD preamplifier module used in GLAS on ICESat: (<b>a</b>) detector module in a 1-inch diameter TO-8 invar metal housing with an optical window; (<b>b</b>) hybrid circuit containing an APD chip, a preamplifier and a high voltage bias regulation circuit; (<b>c</b>) top surface of the active area of the APD with an array of small dimples to deflect the light to increase the photon absorption path length; and (<b>d</b>) enlarged view of the dimple array.</p>
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<p>Photographs of an SPCM used in ICESat/GLAS: (<b>a</b>) detector header with the window removed, showing the silicon APD on top of a TEC and the first stage quenching electronics on a hybrid circuit; (<b>b</b>) SPCM subassembly used in ICESat/GLAS; (<b>c</b>) the power supply and TEC control electronics made by Space Power Electronics, Inc., Bonaire, GA, USA.</p>
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<p>Illustration of HDVIP HgCdTe APD layout and a photograph of the 4 × 4 pixel HgCdTe APD array and ROIC on the chip carrier.</p>
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<p>Spectral response of the 4 × 4 pixel HgCdTe APDs [<a href="#B46-sensors-24-06620" class="html-bibr">46</a>]. The QE is defined as the ratio of the number of output photoelectrons to the number of incident photons at unity APD gain.</p>
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<p>Photographs of the IDCA with the 4 × 4 pixel HgCdTe APD array in a tactical cooler: (<b>a</b>) tactical cooler with the APD array in the Dewar before integration with the external electronics; (<b>b</b>) complete IDCA with the signal buffer amplifiers and detector control electronics on an aluminum support structure.</p>
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<p>Test results of the 2 × 8 pixel IDCA: (<b>a</b>) pulse counts vs. detection threshold from individual pixels in the dark and under illumination at 1.03 μm wavelength; and (<b>b</b>) PDE vs. FER at different detection thresholds. The colors of the curves indicated the outputs from different pixels. The PDE is the ratio of the rate of the net detected photons to the rate of the incident photons. The FER is the rate of the dark counts.</p>
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<p>QE of the analog signal output and maximum PDE from threshold crossing detection of the latest 2 × 8 pixel IDCA measured at 1.55 μm wavelength.</p>
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<p>(<b>a</b>) Impulse response pulse shape; (<b>b</b>) output pulse amplitude vs. the input pulse energy in photons/pulse from the 2 × 8 pixel IDCA at 1.55 μm wavelength.</p>
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<p>(<b>a</b>) Illustration and photograph of the microlens array (MLA) above a 2 × 8 pixel HgCdTe APD array which is also known as focal plane array (FPA); (<b>b</b>) surface scan of a single pixel without the microlens array; and (<b>c</b>) surface scan with the microlens array. The surface scan was performed at 1.03 μm wavelength with a light spot size of about 5 μm.</p>
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<p>Photographs of the 2 × 8 pixel IDCAs: (<b>a</b>) the first generation IDCA designed for CubeSat [<a href="#B51-sensors-24-06620" class="html-bibr">51</a>]; (<b>b</b>) the latest IDCA designed for use in a small lidar. The IDCAs weigh about 0.8 kg with all the peripheral electronics. The cryo-cooler itself consumes about 6 W of electrical power. The electronics consume less than 2 W of power.</p>
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9 pages, 3631 KiB  
Article
Kilowatt-Level High-Efficiency Narrow-Linewidth All-Fiber Tm3+-Doped Laser
by Hongyu Wang, Qilai Zhao, Hang Liu, Yuxin Sun, Jialong Li, Junjie Zheng, Ye Yuan, Qianwen Zhang, Changsheng Yang, Yujun Feng, Yinhong Sun, Zhongmin Yang and Shanhui Xu
Photonics 2024, 11(9), 877; https://doi.org/10.3390/photonics11090877 - 19 Sep 2024
Viewed by 704
Abstract
In this study, a kilowatt-level high-efficiency narrow-linewidth all-fiber Tm3+-doped continuous-wave laser operating at 1.95 μm is demonstrated. Benefitting from an advanced boost design of a two-stage main amplifier, it not only effectively manages heat dissipation resulting from the high pump-induced quantum [...] Read more.
In this study, a kilowatt-level high-efficiency narrow-linewidth all-fiber Tm3+-doped continuous-wave laser operating at 1.95 μm is demonstrated. Benefitting from an advanced boost design of a two-stage main amplifier, it not only effectively manages heat dissipation resulting from the high pump-induced quantum defect but also realizes the controlled extraction of optical gain and improves the optical conversion efficiency. Finally, this laser system has realized an output power of 1018 W, a linewidth of 3.8 GHz, and a slope efficiency of 60.0% simultaneously. Moreover, a high optical signal-to-noise ratio of over 45 dB and excellent beam quality of M2 factors 1.19 are obtained. To the best of our knowledge, this represents the narrowest linewidth and highest slope efficiency achieved in a kilowatt-level Tm³⁺-doped fiber laser. Such a high-performance laser is ideally suited for mid-infrared generation and remote sensing applications. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
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<p>Experimental setup of high-power narrow-linewidth Tm<sup>3+</sup>-doped fiber laser at 1.95 μm. (AWG: arbitrary waveform generator; RF amplifier: radio frequency amplifier; EOM: electro-optic modulators; PA1: 1st pre-amplifier; PA2: 2nd pre-amplifier; MFA: model field adapter; LMA: large-mode-area; TDF: Tm<sup>3+</sup>-doped double-cladding fiber; MM LD: multimode laser diode; CPS: cladding power stripper).</p>
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<p>(<b>a</b>) Spectra of the seed laser with and without phase modulation. Inset: Detailed spectra. (<b>b</b>) Linewidth of the seed laser with phase modulation. Inset: Linewidth of the seed laser without phase modulation.</p>
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<p>(<b>a</b>) Output power variation with pump power in PA2. (<b>b</b>) Optical spectrum of PA2. Inset: Time domain characteristic at 10.6 W output power.</p>
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<p>Variation in output power and backward power with pump power for the 1st main amplifier and the 2nd main amplifier.</p>
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<p>(<b>a</b>) Spectra of the output power at 1018 W. (<b>b</b>) Output signal in time-domain at 1018 W. Inset: Transformed Fourier spectra.</p>
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<p>(<b>a</b>) Measured spectral linewidth at the maximum output power. (<b>b</b>) Measured beam quality factors M<sup>2</sup> at the maximum output power.</p>
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14 pages, 2519 KiB  
Review
Developments of Waveguide Lasers by Femtosecond Laser Direct–Writing Technology
by Yang Zhang, Boyan Yu, Zihao Zhang, Xinghao Duan and Junli Wang
Photonics 2024, 11(9), 803; https://doi.org/10.3390/photonics11090803 - 28 Aug 2024
Viewed by 1035
Abstract
Waveguide lasers have the advantages of miniature and compact structure and have broad application prospects in photonic integration and on–chip laboratories. The development of femtosecond laser direct–writing technology makes the processing of transparent materials more flexible and controllable. This paper mainly introduces a [...] Read more.
Waveguide lasers have the advantages of miniature and compact structure and have broad application prospects in photonic integration and on–chip laboratories. The development of femtosecond laser direct–writing technology makes the processing of transparent materials more flexible and controllable. This paper mainly introduces a waveguide laser based on femtosecond laser direct–writing technology. Firstly, the applications of femtosecond laser direct–writing technology in an optical waveguide are introduced, including the principles of femtosecond laser direct–writing technology, common optical wave scanning methods, and types of optical waveguides. After that, we summarize the development of a waveguide continuous–wave laser, a Q–switched laser and a mode–locked laser from visible to mid–infrared wavebands and analyze some new representative work. Finally, we explain the difficulty of compensating for dispersion in pulse waveguide lasers and summarize some new ideas that have been proposed to solve the problem. Full article
(This article belongs to the Special Issue New Perspectives in Ultrafast Intense Laser Science and Technology)
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<p>Ion exchange technology diagram: (<b>a</b>) thermal ion exchange, (<b>b</b>) field-assisted ion exchange.</p>
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<p>The methods to achieve relative displacement between the laser focus and the sample: (<b>a</b>) sample fixed–laser focus moving method [<a href="#B18-photonics-11-00803" class="html-bibr">18</a>], (<b>b</b>) laser focus fixed–sample moving method [<a href="#B18-photonics-11-00803" class="html-bibr">18</a>]. Waveguide trace writing method: (<b>c</b>) longitudinal scanning method, (<b>d</b>) transverse scanning method.</p>
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<p>Optical microscope pictures of the different waveguide types fabricated in Pr:LLF: (<b>a</b>) circular cladding, (<b>b</b>) ear–like cladding, (<b>c</b>) hexagonal cladding, (<b>d</b>) stress–induced dual–line, (<b>e</b>) stress–induced dual–line with rhombic cladding, (<b>f</b>) single line [<a href="#B58-photonics-11-00803" class="html-bibr">58</a>].</p>
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<p>(<b>a</b>) Experimental setup and (<b>b</b>) output pulse characteristics of Nd:GdVO<sub>4</sub> crystal CW waveguide laser [<a href="#B48-photonics-11-00803" class="html-bibr">48</a>]. WP1 and WP2: waveplate; GTP: Glan Taylor prism; MO: microscope objective lens (20×); CL: convex lens; M1 and M2: laser cavity mirrors adhered to the two end facets of the sample; DB: dichroic beamsplitter; λ<sub>p</sub> and λ<sub>L</sub>: pump and generated laser beam; OC: output coupler.</p>
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<p>The common deposition methods of SA in waveguide lasers: (<b>a</b>) evanescent and (<b>b</b>) direct–field interaction with SA.</p>
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<p>The experimental setup for the Ti:sapphire channel waveguides soliton mode–locking [<a href="#B26-photonics-11-00803" class="html-bibr">26</a>]. DPSS laser: diode–pumped solid–state laser. The green arrow represents the propagation direction of the pump light, while the red arrow represents the propagation direction of the signal light.</p>
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<p>The experimental setup of a Yb:YAG crystal CWML waveguide laser from [<a href="#B65-photonics-11-00803" class="html-bibr">65</a>]. OPSL: optically pumped semiconductor laser; DM: dichroic beamsplitter; L, L1 and L2: lens; OC: output coupler.</p>
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13 pages, 31150 KiB  
Article
Innovative Integration of Dual Quantum Cascade Lasers on Silicon Photonics Platform
by Dongbo Wang, Harindra Kumar Kannojia, Pierre Jouy, Etienne Giraud, Kaspar Suter, Richard Maulini, David Gachet, Léo Hetier, Geert Van Steenberge and Bart Kuyken
Micromachines 2024, 15(8), 1055; https://doi.org/10.3390/mi15081055 - 22 Aug 2024
Viewed by 1202
Abstract
For the first time, we demonstrate the hybrid integration of dual distributed feedback (DFB) quantum cascade lasers (QCLs) on a silicon photonics platform using an innovative 3D self-aligned flip-chip assembly process. The QCL waveguide geometry was predesigned with alignment fiducials, enabling a sub-micron [...] Read more.
For the first time, we demonstrate the hybrid integration of dual distributed feedback (DFB) quantum cascade lasers (QCLs) on a silicon photonics platform using an innovative 3D self-aligned flip-chip assembly process. The QCL waveguide geometry was predesigned with alignment fiducials, enabling a sub-micron accuracy during assembly. Laser oscillation was observed at the designed wavelength of 7.2 μm, with a threshold current of 170 mA at room temperature under pulsed mode operation. The optical output power after an on-chip beam combiner reached sub-milliwatt levels under stable continuous wave operation at 15 °C. The specific packaging design miniaturized the entire light source by a factor of 100 compared with traditional free-space dual lasers module. Divergence values of 2.88 mrad along the horizontal axis and 1.84 mrad along the vertical axis were measured after packaging. Promisingly, adhering to i-line lithography and reducing the reliance on high-end flip-chip tools significantly lowers the cost per chip. This approach opens new avenues for QCL integration on silicon photonic chips, with significant implications for portable mid-infrared spectroscopy devices. Full article
(This article belongs to the Special Issue The 15th Anniversary of Micromachines)
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<p>Schematic representation of the 3D self-alignment flip-chip assembly.</p>
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<p>(<b>a</b>) Simulation of coupling efficiency at different Ge width and gaps, (<b>b</b>) Misalignment simulation, (<b>c</b>) Experimental measurement result of 1 × 2 MMI combiner/splitter, insertion shows the simulated top-view optical profile at 7.2 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m wavelength.</p>
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<p>Process flow for self-assembling QCL on Ge-on-Si PIC.</p>
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<p>SEM images of (<b>a</b>) single mode Ge waveguide, (<b>b</b>) vertical 20 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m deep etched Si recess, (<b>c</b>) Si<sub>3</sub>N<sub>4</sub> AR coating on coupling facet.</p>
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<p>Microscope images of Ge-on-Si PIC (<b>a</b>,<b>b</b>) and InP-based QCL (<b>c</b>), step height profile of Ge-on-Si PIC with ~4 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m thick ENIG layer (<b>d</b>) and QCL (<b>e</b>).</p>
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<p>Stencil alignment step using Tresky’s micro-assembly tool. (<b>a</b>) Top view of stencil aligned on PIC on tacky substrate, (<b>b</b>,<b>c</b>) cross-sectional view before and after alignment, and (<b>d</b>) split-view image of aligned stencil with Ge-on-Si PIC.</p>
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<p>(<b>a</b>,<b>b</b>) Solder imprint area, (<b>c</b>,<b>d</b>) Split-view camera images, (<b>e</b>) Two QCLs integrated on a single Ge-on-Si PIC.</p>
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<p>QCL height on Ge-on-Si PIC (<b>a</b>,<b>b</b>) after flip-chip placement, (<b>c</b>,<b>d</b>) after solder reflow.</p>
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<p>(<b>a</b>) I-V curve at room temperature, (<b>b</b>) optical power under different injection current, insertions show the microscope images during measurement.</p>
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<p>(<b>a</b>) CW operation characterization setup. (<b>b</b>) P-I curve.</p>
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<p>Fully packaged PIC in an HHL module connected to the S2-M driver.</p>
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<p>Lens alignment setup and beam shape after 70 cm of free-space propagation.</p>
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11 pages, 3754 KiB  
Article
Low Dielectric Medium for Hyperbolic Phonon Polariton Waveguide in van der Waals Heterostructures
by Byung-Il Noh, Salvio Reza, Cassie Hardy, Jiahan Li, Adib Taba, Masoud Mahjouri-Samani, James H. Edgar and Siyuan Dai
Nanomaterials 2024, 14(16), 1344; https://doi.org/10.3390/nano14161344 - 14 Aug 2024
Cited by 1 | Viewed by 1083
Abstract
Polar van der Waals (vdW) crystals, composed of atomic layers held together by vdW forces, can host phonon polaritons—quasiparticles arising from the interaction between photons in free-space light and lattice vibrations in polar materials. These crystals offer advantages such as easy fabrication, low [...] Read more.
Polar van der Waals (vdW) crystals, composed of atomic layers held together by vdW forces, can host phonon polaritons—quasiparticles arising from the interaction between photons in free-space light and lattice vibrations in polar materials. These crystals offer advantages such as easy fabrication, low Ohmic loss, and optical confinement. Recently, hexagonal boron nitride (hBN), known for having hyperbolicity in the mid-infrared range, has been used to explore multiple modes with high optical confinement. This opens possibilities for practical polaritonic nanodevices with subdiffractional resolution. However, polariton waves still face exposure to the surrounding environment, leading to significant energy losses. In this work, we propose a simple approach to inducing a hyperbolic phonon polariton (HPhP) waveguide in hBN by incorporating a low dielectric medium, ZrS2. The low dielectric medium serves a dual purpose—it acts as a pathway for polariton propagation, while inducing high optical confinement. We establish the criteria for the HPhP waveguide in vdW heterostructures with various thicknesses of ZrS2 through scattering-type scanning near-field optical microscopy (s-SNOM) and by conducting numerical electromagnetic simulations. Our work presents a feasible and straightforward method for developing practical nanophotonic devices with low optical loss and high confinement, with potential applications such as energy transfer, nano-optical integrated circuits, light trapping, etc. Full article
(This article belongs to the Section Nanophotonics Materials and Devices)
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<p>Schematic illustration and nano-imaging of van der Waals (vdW) heterostructures. (<b>a</b>) Schematics of the experimental setup to image the hyperbolic phonon polariton (HPhP) waveguide with and without low dielectric medium, ZrS<sub>2</sub>. The AFM tip is illuminated by broad mid-infrared (IR) beams from quantum cascade lasers (QCL), which excites HPhP. The back-scattered IR signals are collected to draw s-SNOM images. Experimental s-SNOM images of the vdW heterostructures at the illuminating frequencies ω = 1410 cm<sup>−1</sup> (<b>b</b>) and ω = 1430 cm<sup>−1</sup> (<b>c</b>). The colorful dashed lines correspond to hBN/hBN (black), hBN/43 nm ZrS<sub>2</sub>/hBN (red), and hBN/10 nm ZrS<sub>2</sub>/hBN (blue) regions, respectively.</p>
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<p>HPhP line traces and Fourier Transform (FT) spectra. (<b>a</b>,<b>e</b>) s-SNOM profiles cut along the edge from <a href="#nanomaterials-14-01344-f001" class="html-fig">Figure 1</a>b,c in hBN/hBN, hBN/43 nm ZrS<sub>2</sub>/hBN, and hBN/10 nm ZrS<sub>2</sub>/hBN at ω = 1410 cm<sup>−1</sup> and 1430 cm<sup>−1</sup>. (<b>b</b>–<b>d</b>,<b>f</b>–<b>h</b>) FT spectra of the s-SNOM line profile in (<b>a</b>,<b>e</b>). The two peaks indicate the 1st branch of the edge- and tip-launched hBN mode in the hBN/10 nm ZrS<sub>2</sub>/hBN heterostructure. In the hBN/43 nm ZrS<sub>2</sub>/hBN heterostructure, the FT peaks correspond to the hBN mode and the ZrS<sub>2</sub> waveguide mode (WGM).</p>
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<p>Energy (ω)–momentum (<span class="html-italic">k</span><sub>p</sub>/<span class="html-italic">k</span><sub>0</sub>) dispersions in vdW heterostructures. (<b>a</b>) Schematics of a multilayer system of hBN/ZrS<sub>2</sub>/hBN heterostructures. (<b>b</b>–<b>d</b>) The calculated false-color map is the calculated imaginary reflectivity Im <span class="html-italic">r</span><sub>p</sub> in hBN/hBN, hBN/10 nm ZrS<sub>2</sub>/hBN, and hBN/43 nm ZrS<sub>2</sub>/hBN. The experimental data (red circle) from s-SNOM images and the numerical simulation (blue square) are plotted in the ω − <span class="html-italic">k</span><sub>p</sub>/<span class="html-italic">k</span><sub>0</sub> dispersion.</p>
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<p>Full-wave electromagnetic (EM) numerical simulation of vdW heterostructures. (<b>a</b>–<b>f</b>) The cross-sectional view of the real space images of Re(E<sub>z</sub>) fields on hBN/hBN, hBN/10 nm ZrS<sub>2</sub>/hBN, and hBN/43 nm ZrS<sub>2</sub>/hBN at ω = 1410 (<b>a</b>–<b>c</b>) and 1430 cm<sup>−1</sup> (<b>d</b>–<b>f</b>). Theoretical EM field distribution |E<sub>z</sub>| profiles of hBN/43 nm ZrS<sub>2</sub>/hBN at ω = 1410 (<b>g</b>) and 1430 cm<sup>−1</sup> (<b>h</b>). Shaded areas mark the top hBN (cyan)/middle 43 nm ZrS<sub>2</sub> (yellow)/bottom hBN (green), respectively. (<b>i</b>) The dependence of the theoretical HPhP wavelength <span class="html-italic">λ</span><sub>p</sub> on the frequency ω.</p>
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12 pages, 3384 KiB  
Article
A Mid-Infrared Perfect Metasurface Absorber with Tri-Band Broadband Scalability
by Yongtu Zou, Shaolin Zhou, Jingxi Li, Shanri Chen and Zhijian Chen
Nanomaterials 2024, 14(15), 1316; https://doi.org/10.3390/nano14151316 - 5 Aug 2024
Cited by 1 | Viewed by 1362
Abstract
Metasurfaces have emerged as a unique group of two-dimensional ultra-compact subwavelength devices for perfect wave absorption due to their exceptional capabilities of light modulation. Nonetheless, achieving high absorption, particularly with multi-band broadband scalability for specialized scenarios, remains a challenge. As an example, the [...] Read more.
Metasurfaces have emerged as a unique group of two-dimensional ultra-compact subwavelength devices for perfect wave absorption due to their exceptional capabilities of light modulation. Nonetheless, achieving high absorption, particularly with multi-band broadband scalability for specialized scenarios, remains a challenge. As an example, the presence of atmospheric windows, as dictated by special gas molecules in different infrared regions, highly demands such scalable modulation abilities for multi-band absorption and filtration. Herein, by leveraging the hybrid effect of Fabry–Perot resonance, magnetic dipole resonance and electric dipole resonance, we achieved multi-broadband absorptivity in three prominent infrared atmospheric windows concurrently, with an average absorptivity of 87.6% in the short-wave infrared region (1.4–1.7 μm), 92.7% in the mid-wave infrared region (3.2–5 μm) and 92.4% in the long-wave infrared region (8–13 μm), respectively. The well-confirmed absorption spectra along with its adaptation to varied incident angles and polarization angles of radiations reveal great potential for fields like infrared imaging, photodetection and communication. Full article
(This article belongs to the Special Issue Nonlinear Optics of Nanostructures and Metasurfaces)
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<p>Schematic of metasurface absorbers constructed using three different types of nanoresonators: (<b>a</b>) a Cr patch, with period of p = 1.8 μm, length of patch l = 1.6 μm, thickness of t<sub>m</sub> = 200 nm, on a dielectric spacer with thickness t<sub>d</sub> = 600 nm and a bottom metal substrate thickness of t<sub>s</sub> = 100 nm; (<b>b</b>) a Au patch with the same as that in the (<b>a</b>); (<b>c</b>) Ge Cube, with a period of 2.8 μm and length and thicknesses of <span class="html-italic">l</span> = 2.1 μm, t<sub>i</sub> = 2.1 μm, t<sub>d</sub> = 2.4 μm, t<sub>s</sub> = 100 nm. (<b>d</b>) Calculated infrared absorption spectra (left axis) of the MSA with a Cr patch, Au patch and Ge cube. The extinction coefficient of Au and Cr are cited from [<a href="#B38-nanomaterials-14-01316" class="html-bibr">38</a>,<a href="#B39-nanomaterials-14-01316" class="html-bibr">39</a>] (right axis). Intrinsic Ge is lossless with a negligible extinction coefficient [<a href="#B40-nanomaterials-14-01316" class="html-bibr">40</a>].</p>
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<p>(<b>a</b>) The schematic of multi-mode coupling for broadband modulations of multi-band absorption. (<b>b</b>) The absorption spectrum of the MSA in <a href="#nanomaterials-14-01316-f001" class="html-fig">Figure 1</a> with parameters of <span class="html-italic">p</span> = 3 μm, <span class="html-italic">l</span> = 2 μm, <span class="html-italic">t<sub>m</sub></span> = 300 nm, t<sub>d</sub> = 0.9 μm, and <span class="html-italic">t<sub>s</sub></span> = 100 nm and electric intensity profiles in the YOZ plane at wavelengths of (<b>c</b>) λ<sub>1</sub> = 3.26 μm, (<b>d</b>) λ<sub>2</sub> = 3.95 μm, and (<b>e</b>) λ<sub>3</sub> = 8.97 μm.</p>
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<p>The schematic of the proposed MSA: (<b>a</b>) oblique view; (<b>b</b>) vertical view; (<b>c</b>) the absorption spectrum in the infrared region.</p>
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<p>The electric field intensity profiles extracted in the XOY plane at seven resonance peaks at (<b>a</b>) λ<sub>1</sub> = 1.57 μm, (<b>b</b>) λ<sub>2</sub> = 3.68 μm, (<b>c</b>) λ<sub>3</sub> = 4.64 μm, (<b>d</b>) λ<sub>4</sub> = 8.39 μm, (<b>e</b>) λ<sub>5</sub> = 9.22 μm, (<b>f</b>) λ<sub>6</sub> = 10.61 μm and (<b>g</b>) λ<sub>7</sub> = 11.94 μm. All electric field intensity profiles use the same reference scale.</p>
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<p>The absorption spectra extracted under a parameter sweep with varying (<b>a</b>) patch length <span class="html-italic">l</span><sub>1</sub>, (<b>b</b>) patch length <span class="html-italic">l</span><sub>4</sub>, (<b>c</b>) grid width <span class="html-italic">w</span> and (<b>d</b>) CaF<sub>2</sub> thickness <span class="html-italic">t<sub>d</sub></span>.</p>
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<p>The absorption color maps obtained by different (<b>a</b>) polarization angles and (<b>b</b>) incident angles of TE incidence and (<b>c</b>) polarization angles and (<b>d</b>) incident angles of TM incidence.</p>
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<p>(<b>a</b>) The schematic of a single patch–grid structure. The structural parameters are as follows: p = 4 μm, l = 1.7 μm, t<sub>m</sub> = 300 nm, t<sub>d</sub> = 0.9 μm, t<sub>m</sub> = 150 nm, w = 0.4 μm. (<b>b</b>) The absorption spectrum with different patch lengths.</p>
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<p>The absorption spectra of three types of MSA configured by different nanoresonators in the top layer. The setup using only the grid or only the patch shares the same parameters with our tri-band broadband MSA.</p>
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17 pages, 32143 KiB  
Article
MWIRGas-YOLO: Gas Leakage Detection Based on Mid-Wave Infrared Imaging
by Shiwei Xu, Xia Wang, Qiyang Sun and Kangjun Dong
Sensors 2024, 24(13), 4345; https://doi.org/10.3390/s24134345 - 4 Jul 2024
Viewed by 1364
Abstract
The integration of visual algorithms with infrared imaging technology has become an effective tool for industrial gas leak detection. However, existing research has mostly focused on simple scenarios where a gas plume is clearly visible, with limited studies on detecting gas in complex [...] Read more.
The integration of visual algorithms with infrared imaging technology has become an effective tool for industrial gas leak detection. However, existing research has mostly focused on simple scenarios where a gas plume is clearly visible, with limited studies on detecting gas in complex scenes where target contours are blurred and contrast is low. This paper uses a cooled mid-wave infrared (MWIR) system to provide high sensitivity and fast response imaging and proposes the MWIRGas-YOLO network for detecting gas leaks in mid-wave infrared imaging. This network effectively detects low-contrast gas leakage and segments the gas plume within the scene. In MWIRGas-YOLO, it utilizes the global attention mechanism (GAM) to fully focus on gas plume targets during feature fusion, adds a small target detection layer to enhance information on small-sized targets, and employs transfer learning of similar features from visible light smoke to provide the model with prior knowledge of infrared gas features. Using a cooled mid-wave infrared imager to collect gas leak images, the experimental results show that the proposed algorithm significantly improves the performance over the original model. The segment mean average precision reached 96.1% (mAP50) and 47.6% (mAP50:95), respectively, outperforming the other mainstream algorithms. This can provide an effective reference for research on infrared imaging for gas leak detection. Full article
(This article belongs to the Section Sensing and Imaging)
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<p>Three-layer radiation transfer model and gas infrared imaging detection system. <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">M</mi> <mrow> <mi>B</mi> <mi>G</mi> </mrow> </msub> </semantics></math> is the background spectral radiation, <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">M</mi> <mrow> <mi>l</mi> <mi>e</mi> <mi>a</mi> <mi>k</mi> </mrow> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">M</mi> <mrow> <mi>n</mi> <mi>o</mi> <mo>_</mo> <mi>l</mi> <mi>e</mi> <mi>a</mi> <mi>k</mi> </mrow> </msub> </semantics></math> are gas path and non-gas path radiation.</p>
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<p>Infrared gas image samples.The red bounding box represents the leaked gas. Below the image are the leak distance, gas type, and leak rate.</p>
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<p>Infrared gas images categorized into three types; the top left of the image shows enlarged views of the gas region image and its corresponding frame difference image. (<b>a</b>) Dense, where the gas plume in the scene is easily observable at a glance. (<b>b</b>) Thin, requiring careful observation of local areas to detect the gas plume. (<b>c</b>) Indiscernible, where the gas plume cannot be directly observed in a single frame and requires observation of multiple frames before and after to identify its position.</p>
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<p>Histogram of mask pixel count. A mask pixel count ranging from 65 to 475 in a single image is considered a small object.</p>
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<p>MWIRGas-YOLO network architecture.</p>
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<p>Channel attention submodule.</p>
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<p>Spatial attention submodule.</p>
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<p>Global attention mechanism.</p>
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<p>Prior model detection results. (<b>a</b>) Visible smoke image detection results. (<b>b</b>) Infrared gas image detection results.</p>
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<p>The feature map before and after embedding GAM, and the red bounding box is the activation of the target feature. (<b>a</b>) Results of backbone comparison. (<b>b</b>) Results of neck comparison.</p>
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<p>Test comparison diagram. (<b>a</b>) YOLOv8-seg test result. (<b>b</b>) MWIRGas-YOLO test result.</p>
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<p>Visual comparison of training process. (<b>a</b>) Precision curve. (<b>b</b>) Recall curve. (<b>c</b>) mAP50 curve. (<b>d</b>) mAP50:95 curve.</p>
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<p>Visualization of detection and segmentation results by different methods on MWIRGas-Seg dataset.</p>
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17 pages, 5481 KiB  
Article
Reach-Scale Mapping of Surface Flow Velocities from Thermal Images Acquired by an Uncrewed Aircraft System along the Sacramento River, California, USA
by Paul J. Kinzel, Carl J. Legleiter and Christopher L. Gazoorian
Water 2024, 16(13), 1870; https://doi.org/10.3390/w16131870 - 29 Jun 2024
Viewed by 936
Abstract
An innovative payload containing a sensitive mid-wave infrared camera was flown on an uncrewed aircraft system (UAS) to acquire thermal imagery along a reach of the Sacramento River, California, USA. The imagery was used as input for an ensemble particle image velocimetry (PIV) [...] Read more.
An innovative payload containing a sensitive mid-wave infrared camera was flown on an uncrewed aircraft system (UAS) to acquire thermal imagery along a reach of the Sacramento River, California, USA. The imagery was used as input for an ensemble particle image velocimetry (PIV) algorithm to produce near-continuous maps of surface flow velocity along a reach approximately 1 km in length. To assess the accuracy of PIV velocity estimates, in situ measurements of flow velocity were obtained with an acoustic Doppler current profiler (ADCP). ADCP measurements were collected along pre-planned cross-section lines within the area covered by the imagery. The PIV velocities showed good agreement with the depth-averaged velocity measured by the ADCP, with R2 values ranging from 0.59–0.97 across eight transects. Velocity maps derived from the thermal image sequences acquired on consecutive days during a period of steady flow were compared. These maps showed consistent spatial patterns of velocity vector magnitude and orientation, indicating that the technique is repeatable and robust. PIV of thermal imagery can yield velocity estimates in situations where natural water-surface textures or tracers are either insufficient or absent in visible imagery. Future work could be directed toward defining optimal environmental conditions, as well as limitations for mapping flow velocities based on thermal images acquired via UAS. Full article
(This article belongs to the Section Biodiversity and Functionality of Aquatic Ecosystems)
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<p>Aerial orthophotograph of the study reach along the Sacramento River showing the cross-section locations corresponding to UAS-based image acquisition and ADCP velocity measurements.</p>
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<p>Air and water temperatures at the time of UAS flights, ADCP data collection, and streamflow at USGS streamgage 11389500, Sacramento River at Colusa [<a href="#B35-water-16-01870" class="html-bibr">35</a>].</p>
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<p>Images of the DJI Matrice 600 Pro hexacopter equipped with the River Observing System (RiOS) payload. Photographs by Massimo Vespignani, NASA, used with permission.</p>
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<p>Data acquisition, image processing, and PIV workflow.</p>
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<p>(<b>a</b>) Unprocessed and (<b>b</b>) processed thermal image of the Sacramento River.</p>
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<p>Reach-level comparison of ADCP depth-averaged velocities with thermal PIV-derived surface velocities for (<b>a</b>) 9 November and (<b>b</b>) 10 November. The solid line is the regression line and the dashed line is the 1:1 line.</p>
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<p>Reach-scale velocity maps for 9 November (<b>a</b>) and 10 November (<b>b</b>).</p>
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<p>Observed versus predicted plot for velocity fields from 9 November and 10 November. The solid line is the regression line, and the dashed line is the 1:1 line.</p>
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<p>Comparison of vector fields from 9 November and 10 November.</p>
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15 pages, 3463 KiB  
Article
Design Considerations for Continuous Wave Intracavity Backwards Optical Parametric Oscillators
by Josh Kneller, Liam Flannigan and Chang-Qing Xu
Photonics 2024, 11(4), 318; https://doi.org/10.3390/photonics11040318 - 29 Mar 2024
Cited by 1 | Viewed by 870
Abstract
In this paper, we report a theoretical systematic study of continuous wave intracavity backwards optical parametric oscillators based on periodically poled lithium niobate (PPLN) for mid-infrared (mid-IR) light generation. We study the effects of varying different cavity parameters including nonlinear crystal length, cavity [...] Read more.
In this paper, we report a theoretical systematic study of continuous wave intracavity backwards optical parametric oscillators based on periodically poled lithium niobate (PPLN) for mid-infrared (mid-IR) light generation. We study the effects of varying different cavity parameters including nonlinear crystal length, cavity size, pump laser diode spot size, output coupler radius, and cavity loss values on the output power and threshold of the proposed mid-IR laser. The effects of different physical phenomena are included in the model including pump depletion due to the nonlinear conversion process, the thermal lens effect, and mode overlap between the beams in the nonlinear crystal. We show that high output powers in the mid infrared (>500 mW at 3.2 μm) can be achieved with proper cavity design and that a laser threshold with a PPLN as short as 2 cm can be reached. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
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<p>Design of proposed mid-IR source. Coatings are shown in orange and numbered.</p>
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<p>Maximum output idler power for different cavity spacings with a 5 cm PPLN.</p>
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<p>Threshold for a 5 cm PPLN at various cavity spacings.</p>
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<p>Output power for different PPLN lengths with a constant cavity size.</p>
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<p>Pump beam radius for a 5 cm PPLN at different D1 values and input LD beam waists.</p>
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<p>Dependence of output power on the pump beam radius in the PPLN for different LD beam waists.</p>
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<p>Idler power for a 5 cm PPLN with different OC radii.</p>
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<p>Idler power for a 3 cm PPLN with different OC radii.</p>
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<p>Output power for a 5 cm PPLN with a 50 mm radius at different 808 nm LD beam waists.</p>
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<p>Maximum output power for different PPLN lengths at various LD beam waists with a 50 mm OC.</p>
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<p>Output power for 5cm PPLN at different signal and pump cavity loss values.</p>
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<p>Output power achievable with and without a dichroic mirror for different mirror loss values.</p>
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12 pages, 3365 KiB  
Article
Bias-Tunable Quantum Well Infrared Photodetector
by Gyana Biswal, Michael Yakimov, Vadim Tokranov, Kimberly Sablon, Sergey Tulyakov, Vladimir Mitin and Serge Oktyabrsky
Nanomaterials 2024, 14(6), 548; https://doi.org/10.3390/nano14060548 - 20 Mar 2024
Cited by 1 | Viewed by 1408
Abstract
With the rapid advancement of Artificial Intelligence-driven object recognition, the development of cognitive tunable imaging sensors has become a critically important field. In this paper, we demonstrate an infrared (IR) sensor with spectral tunability controlled by the applied bias between the long-wave and [...] Read more.
With the rapid advancement of Artificial Intelligence-driven object recognition, the development of cognitive tunable imaging sensors has become a critically important field. In this paper, we demonstrate an infrared (IR) sensor with spectral tunability controlled by the applied bias between the long-wave and mid-wave IR spectral regions. The sensor is a Quantum Well Infrared Photodetector (QWIP) containing asymmetrically doped double QWs where the external electric field alters the electron population in the wells and hence spectral responsivity. The design rules are obtained by calculating the electronic transition energies for symmetric and antisymmetric double-QW states using a Schrödinger–Poisson solver. The sensor is grown and characterized aiming detection in mid-wave (~5 µm) to long-wave IR (~8 µm) spectral ranges. The structure is grown using molecular beam epitaxy (MBE) and contains 25 periods of coupled double GaAs QWs and Al0.38Ga0.62As barriers. One of the QWs in the pair is modulation-doped to provide asymmetry in potential. The QWIPs are tested with blackbody radiation and FTIR down to 77 K. As a result, the ratio of the responsivities of the two bands at about 5.5 and 8 µm is controlled over an order of magnitude demonstrating tunability between MWIR and LWIR spectral regions. Separate experiments using parameterized image transformations of wideband LWIR imagery are performed to lay the framework for utilizing tunable QWIP sensors in object recognition applications. Full article
(This article belongs to the Special Issue Graphene-Based Optoelectronic and Plasmonic Devices)
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<p>Calculated localized energy states and corresponding wavefunctions (<math display="inline"><semantics> <mrow> <msup> <mrow> <mfenced open="|" close="|" separators="|"> <mrow> <mi>ψ</mi> </mrow> </mfenced> </mrow> <mrow> <mn>2</mn> </mrow> </msup> </mrow> </semantics></math>) in the double QW structure at 77 K under (<b>a</b>) −3 V, (<b>b</b>) 0 V, and (<b>c</b>) +3 V bias. Zero energy corresponds to the Fermi level position. Four transitions are indicated by arrows with the letters “A” to “D” assigned from low to high energies. Structure parameters: QW width, 6 nm; Al content in the barrier, 0.35; barrier width between the coupled wells, 2.5 nm; electron concentration, 5 × 10<sup>11</sup> cm<sup>−2</sup>.</p>
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<p>Transition energy and corresponding wavelength (<b>a</b>) vs. the internal barrier width in the double QW structure; (<b>b</b>) vs. the internal barrier at a constant thickness (2.5 nm); and (<b>c</b>) Al concentration in the barrier.</p>
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<p>(<b>a</b>) Schematic epitaxial structure of the MBE-grown QWIP with asymmetrically doped double QWs. (<b>b</b>) High-resolution TEM image of a single detection unit showing GaAs and AlGaAs layers. GaAs appears darker than AlGaAs due to stronger electron scattering. (<b>c</b>) Intensity map across the structure to estimate thicknesses.</p>
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<p>(<b>a</b>) Temperature dependence of the dark current in a 300 × 300 µm<sup>2</sup> QWIP from 77 K to 170 K. (<b>b</b>) Activation energy vs. bias from Arrhenius plot for the QWIP.</p>
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<p>(<b>a</b>) Experimental FTIR spectral response of 25-period QWIP at 77 K as a function of applied bias for positive and negative polarities compared with transition energies obtained from the simulation in <a href="#nanomaterials-14-00548-f001" class="html-fig">Figure 1</a>. The transitions are indicated by wide lines extended to higher energies qualitatively resembling the spreading of the electrons in the respective subbands. Transistions “A” to “D” are indicated in <a href="#nanomaterials-14-00548-f001" class="html-fig">Figure 1</a>. (<b>b</b>) Integral response of the two bands controlled by the applied bias to the QWIP structure and the response ratio of the two bands at 5.5 µm and 8 µm.</p>
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<p>Examples of 8-bit images obtained by parameterized transformations from raw 16-bit images.</p>
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21 pages, 7838 KiB  
Review
Applications of Microstructured Optical Fibers in Ultrafast Optics: A Review
by Ziwen Tang, Zihua Zheng, Boyao Li, Zhiyi Wei and Jinghua Sun
Photonics 2024, 11(2), 151; https://doi.org/10.3390/photonics11020151 - 5 Feb 2024
Cited by 3 | Viewed by 2099
Abstract
With the development of laser technology, microstructured optical fibers (MOFs) have become an important part of ultrafast optics, providing excellent platforms for ultrafast laser pulse generation, amplification, and compression, promoting the development of fiber laser systems to generate high power, high pulse energy, [...] Read more.
With the development of laser technology, microstructured optical fibers (MOFs) have become an important part of ultrafast optics, providing excellent platforms for ultrafast laser pulse generation, amplification, and compression, promoting the development of fiber laser systems to generate high power, high pulse energy, and few-cycle duration pulses. MOFs extend the ultrafast laser spectrum to the vacuum ultraviolet (VUV) and even extreme ultraviolet (EUV) regions based on dispersive wave emission and high harmonic generation, as well as to the mid-infrared region based on soliton self-frequency shift (SSFS), contributing compact and low-cost light sources for precision microscopy and spectroscopy. In this paper, first several common types of MOFs are introduced, then the various applications of MOFs in ultrafast optics are discussed, mainly focusing on the aspects of ultrafast laser pulse scaling in pulse energy and spectral bandwidth, and finally the possible prospects of MOFs are given. Full article
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<p>Scanning electron microscope (SEM) images of the cross-section of the solid-core PCFs. (<b>a</b>) The first solid PCF [<a href="#B19-photonics-11-00151" class="html-bibr">19</a>]; (<b>b</b>) Four-core PCF [<a href="#B20-photonics-11-00151" class="html-bibr">20</a>]; (<b>c</b>) Multi-core PCF [<a href="#B21-photonics-11-00151" class="html-bibr">21</a>].</p>
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<p>SEM images of the cross section of the PBGFs. (<b>a</b>) The first honeycomb structure PBGF [<a href="#B23-photonics-11-00151" class="html-bibr">23</a>]; (<b>b</b>) All-solid PBGF (Ge-doped capillary rods inserted in the silica substrate) [<a href="#B24-photonics-11-00151" class="html-bibr">24</a>]; (<b>c</b>) The first HC-PBGF [<a href="#B25-photonics-11-00151" class="html-bibr">25</a>]; (<b>d</b>) Kagome HC-PCF [<a href="#B26-photonics-11-00151" class="html-bibr">26</a>]. (The core diameters of these PBGFs are (<b>a</b>) 0.8 μm, (<b>b</b>) 39.5 μm, (<b>c</b>) 14.8 μm, and (<b>d</b>) 170 μm).</p>
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<p>Guidance mechanisms of (<b>a</b>) Frustrated tunneling PBG effect and (<b>b</b>) Bragg PBG effect [<a href="#B25-photonics-11-00151" class="html-bibr">25</a>].</p>
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<p>SEM image of the cross-section of the ARFs. (<b>a</b>) Single ring ARF with touching point [<a href="#B28-photonics-11-00151" class="html-bibr">28</a>], (core diameter is 36 μm, the outer diameter of the single ring is 22.5 μm, inner diameter is 17.1 μm); (<b>b</b>) Conjoined-tube ARF [<a href="#B29-photonics-11-00151" class="html-bibr">29</a>], (core diameter is 30.5 μm, the yellow numbers label the five dielectric layers in the cladding); (<b>c</b>) Nested ARF [<a href="#B30-photonics-11-00151" class="html-bibr">30</a>], (core diameter is 32.5 μm, outer diameter is 25.6 μm, inner diameter is 12.1 μm).</p>
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<p>The guidance mechanism of ARF (equivalent Fabry–Perot cavity model).</p>
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<p>SEM image of the cross-section of the first Hybrid PCF [<a href="#B33-photonics-11-00151" class="html-bibr">33</a>]. The hybrid PCF is composed of air holes (black) and Ge-doped silica rods (gray rods in horizontal direction) disposed around an undoped silica core.</p>
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<p>Schematic diagram of CPA technology.</p>
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<p>(<b>a</b>) Schematic of the coherently combined fiber CPA laser system [<a href="#B41-photonics-11-00151" class="html-bibr">41</a>] (CFBG, chirped fiber Bragg gratings; FDPS, Fourier-domain pulse shaper; AOM, acousto-optic modulator; LPF, large-pitch fiber; QWP, quarter-wave plate; HWP, half-wave plate; PBS, polarizing beam splitter; TFP, thin-film polarizer); (<b>b</b>) SEM image of the cross-section of the LPF [<a href="#B44-photonics-11-00151" class="html-bibr">44</a>] (the core diameter is 135 μm).</p>
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<p>Experimental spectra of SCG. The blue curve was measured by the VUV spectrometer, and the brown curve was UV-NIR spectrometer. The solid black line is the simulated spectrum. The dashed vertical line marks the ZDW (N = normal, A = anomalous GVD) [<a href="#B60-photonics-11-00151" class="html-bibr">60</a>].</p>
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<p>Experimental setup of the compact SC source [<a href="#B67-photonics-11-00151" class="html-bibr">67</a>] (EDF: Erbium-doped fiber; GSA: graphene saturable absorber; OC: output coupler; ISO: isolator; WDM: wavelength division multiplexer; PM-HNLF: polarization maintaining highly nonlinear fiber).</p>
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<p>(<b>a</b>) SEM image of the cross section of the kagome-type HC-PCF used for HHG, where the effective mode diameter (corresponding to the hollow center core) is about 15 μm; (<b>b</b>) Measured spectrum of the HHG [<a href="#B76-photonics-11-00151" class="html-bibr">76</a>].</p>
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<p>Experimental generation of coherent ultrashort pulses through resonant dispersive wave emission in gas-filled kagome HC-PCF [<a href="#B81-photonics-11-00151" class="html-bibr">81</a>]. Each peak is the individual normalized spectrum for a specific gas, pressure, and pump energy. All the tuning was carried out in an identical length of kagomé HC-PCF (27 µm core diameter), except in the case of neon, where the core diameter was 37 µm.</p>
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<p>(<b>a</b>) Experimental setup of the two-stage ARF compressor. <span class="html-italic">λ</span>/2: half-wave plate. <span class="html-italic">λ</span>/4: quarter-wave plate. TFP: thin-film polarizer. CM: negatively chirped mirror. FM: flip mirror. OAPM: off-axis parabolic mirror. W: glass wedge. (<b>b</b>,<b>c</b>) SEM images of the ARFs, core diameters 86 µm in the first compression stage and 59 µm in the second stage [<a href="#B103-photonics-11-00151" class="html-bibr">103</a>].</p>
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<p>(<b>a</b>) Experiment setup of HHML for high repetition rate soliton generation, LD: laser diode, ISO: isolator, PC: polarization controller, SMF: single mode fiber; (<b>b</b>) <b>left</b>: SEM of the solid-core PCF, <b>right</b>: zoom-in of the core region. The two slightly smaller hollow channels marked by the red arrows render the PCF polarization-maintaining [<a href="#B112-photonics-11-00151" class="html-bibr">112</a>].</p>
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14 pages, 4544 KiB  
Article
InAsSb Photodiode Fibre Optic Thermometry for High-Speed, near-Ambient Temperature Measurements
by Emilios Leonidas, Matthew J. Hobbs, Sabino Ayvar-Soberanis, Hatim Laalej, Callum Fisk, Stephen Fitzpatrick and Jon R. Willmott
Sensors 2023, 23(23), 9514; https://doi.org/10.3390/s23239514 - 30 Nov 2023
Viewed by 1429
Abstract
Infrared radiation thermometers (IRTs) overcome many of the limitations of thermocouples, particularly responsiveness and calibration drift. The main challenge with radiation thermometry is the fast and reliable measurement of temperatures close to room temperature. A new IRT which is sensitive to wavelengths between [...] Read more.
Infrared radiation thermometers (IRTs) overcome many of the limitations of thermocouples, particularly responsiveness and calibration drift. The main challenge with radiation thermometry is the fast and reliable measurement of temperatures close to room temperature. A new IRT which is sensitive to wavelengths between 3 μm and 11 μm was developed and tested in a laboratory setting. It is based on an uncooled indium arsenide antimony (InAsSb) photodiode, a transimpedance amplifier, and a silver halogenide fibre optic cable transmissive in the mid- to long-wave infrared region. The prototype IRT was capable of measuring temperatures between 35 °C and 100 °C at an integration time of 5 ms and a temperature range between 40 °C and 100 °C at an integration time of 1 ms, with a root mean square (RMS) noise level of less than 0.5 °C. The thermometer was calibrated against Planck’s law using a five-point calibration, leading to a measurement uncertainty within ±1.5 °C over the aforementioned temperature range. The thermometer was tested against a thermocouple during drilling operations of polyether ether ketone (PEEK) plastic to measure the temperature of the drill bit during the material removal process. Future versions of the thermometer are intended to be used as a thermocouple replacement in high-speed, near-ambient temperature measurement applications, such as electric motor condition monitoring; battery protection; and machining of polymers and composite materials, such as carbon-fibre-reinforced plastic (CFRP). Full article
(This article belongs to the Special Issue Advances in Applications of Optical Fiber Sensors)
Show Figures

Figure 1

Figure 1
<p>InAsSb photodiode transimpedance amplifier schematic.</p>
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<p>Configuration of the experimental apparatus used for the IRT characterisation.</p>
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<p>Response time measurement apparatus configuration.</p>
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<p>Infrared radiation thermometry calibration steps (<b>a</b>–<b>d</b>) (based on Hobbs et al. [<a href="#B31-sensors-23-09514" class="html-bibr">31</a>]).</p>
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<p>(<b>a</b>) Aluminium disc with blind holes and dimensions; (<b>b</b>) schematic of the embedded thermocouples inside the blind holes.</p>
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<p>RMS noise as a function of target temperature for integration times of 400 μs, 1 ms, 5 ms, and 10 ms for the IRT and 10 ms for the thermocouple.</p>
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<p>Rise time assessment of the IRT with an optical chopper at a frequency of 500 Hz at a target temperature of 80 °C.</p>
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<p>(<b>a</b>) Output voltage as a function of target temperature; (<b>b</b>) characteristic inverse absolute temperature against the natural logarithm of the output voltage.</p>
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<p>(<b>a</b>) Calculated and measured output voltages against temperature (calibration); (<b>b</b>) instrument error after calibration compared to the thermocouple tolerance bounds for Class 1 and Class 2 tolerances.</p>
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<p>IRT temperature against time for acquisition times of 400 μs, 1 ms, 5 ms, and 10 ms for a target temperature.</p>
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<p>Arrangement of the IRT and thermocouple inside the PEEK workpiece during drilling operations on a manual milling machine.</p>
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<p>IRT and thermocouple temperature measurements during drilling operations.</p>
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