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Search Results (929)

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14 pages, 6268 KiB  
Article
Analysis of Influence of Abnormal Fiber-Optical Current Transformer on Double Closed-Loop Control of Converter Valve in Flexible DC Converter Station
by Yirun Ji, Qing Huai, Xuanfei Huang, Libo Ma, Qian Yuan, Chengjie Zhou and Chen Zhao
Electronics 2025, 14(1), 141; https://doi.org/10.3390/electronics14010141 - 1 Jan 2025
Viewed by 361
Abstract
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter [...] Read more.
The fiber-optical current transformer (FOCT) is the core measuring equipment of the flexible DC converter station, which affects the operation control of the system. In order to solve the problem of the influence of the abnormal FOCT on the operation of the converter valve being unclear, the common fault modes of temperature and optical path of the FOCT are analyzed in this paper. Then, based on the traditional optical current transformer (OCT) model and considering the influence of temperature parameters on the FOCT, the FOCT dynamic model considering multiple factors is constructed. Finally, the simulation analysis is carried out on the MATLAB 2021b/Simulink platform, and the results show that (1) when the FOCT temperature compensation is abnormal, the transmission power of the converter valve increases with the increase in temperature, but the increase in temperature change is small; (2) when the FOCT light source compensation is abnormal, the light source attenuates, the converter valve active power decreases, and the reactive power increases; and (3) when the optical fiber sensing ring is broken, the transmission power increases and seriously deviates from the preset value (the active power increases by about 87.5% and the reactive power increases by about 90%). It can be seen that the abnormal FOCT in the converter station has a serious influence on the operation of the converter valve. Full article
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<p>Schematic diagram of FOCT.</p>
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<p>Three-phase MMC topology.</p>
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<p>Coupled model of flexible DC converter valve and FOCT.</p>
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<p>Model and measured current values.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>AC current runs on the rectification side.</p>
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<p>Active power.</p>
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<p>Reactive power.</p>
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<p>Overall block diagram of the system.</p>
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<p>Detailed diagram of FOCT simulation module.</p>
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<p>Detailed diagram of outer-loop power control module.</p>
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<p>Detailed diagram of inner-loop current control module.</p>
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20 pages, 7540 KiB  
Article
Investigation into the Synergistic Effects of Sediment Concentration and Particle Size on the Friction and Wear Properties of Nitrile Butadiene Rubber
by Lun Wang, Xincong Zhou, Qipeng Huang, Xueshen Liu, Zhenjiang Zhou and Shaopeng Xing
J. Mar. Sci. Eng. 2025, 13(1), 33; https://doi.org/10.3390/jmse13010033 - 29 Dec 2024
Viewed by 340
Abstract
Nitrile Butadiene Rubber (NBR) is commonly used in ships’ water-lubricated tail bearings. However, sediment in the water significantly affects these bearings’ friction and wear performance. This study investigates NBR test blocks’ friction and wear behavior in conjunction with ZCuSn10Zn2 copper ring friction pairs [...] Read more.
Nitrile Butadiene Rubber (NBR) is commonly used in ships’ water-lubricated tail bearings. However, sediment in the water significantly affects these bearings’ friction and wear performance. This study investigates NBR test blocks’ friction and wear behavior in conjunction with ZCuSn10Zn2 copper ring friction pairs within a sediment-laden water lubrication environment. Two primary factors were considered: sediment particle concentration and sediment particle size. Friction and wear tests were conducted under pure water and sediment-laden conditions using the ZY-1 ring block friction and wear tester. The friction coefficients, wear quantities, and variations in mass concentrations and sediment particle sizes were measured and compared. The surface morphology of the test blocks was analyzed using a laser confocal microscope. The findings indicate that as sediment concentration increases, the particle size’s impact on NBR’s abrasive wear diminishes. The variation in particle size directly influences the number of particles that penetrate the interface between the friction partners and the nature of three-body wear. Conversely, changes in particle concentration primarily affect the extent of wear; specifically, both the wear volume and the average coefficient of friction of the NBR specimens increase with rising sediment concentration. The wear mechanisms observed on the surface of the NBR test blocks are predominantly characterized by micro-cutting, rolling wear, and the coexistence of both wear modes. This study offers valuable insights for the design and optimization of water-lubricated bearings. Full article
(This article belongs to the Section Ocean Engineering)
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<p>Schematic diagram of test materials. (<b>a</b>) NBR test block sample, (<b>b</b>) copper ring sample, (<b>c</b>) SiO<sub>2</sub> powder sample, (<b>d</b>) solution.</p>
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<p>Typical micrographs of four sediment particles of different sizes.</p>
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<p>Schematic diagram of friction wear tester. (<b>a</b>) Schematic diagram of the testing machine, (<b>b</b>) principle diagram of the loading mechanism.</p>
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<p>Average friction coefficient variation results of NBR specimens under different loads and sliding velocities.</p>
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<p>Friction coefficient results under the influence of particle size.</p>
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<p>Wear volume under the influence of particle size. (<b>a</b>) At 1.5% sediment concentration, (<b>b</b>) at 3% sediment concentration, (<b>c</b>) at 4.5% sediment concentration, (<b>d</b>) at 6% sediment concentration, (<b>e</b>) at 7.5% sediment concentration, (<b>f</b>) at 9% sediment concentration.</p>
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<p>Wear surface morphology under the influence of particle size. (<b>a</b>) At particle size 5 μm, (<b>b</b>) at particle size 15 μm, (<b>c</b>) at particle size 25 μm, (<b>d</b>) at particle size 38 μm, (<b>e</b>) at particle size 45 μm, (<b>f</b>) at particle size 75 μm.</p>
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<p>Wear mechanism diagram of NBR under the influence of particle size. (<b>a</b>) NBR wear mechanism diagram under the influence of small size particles, (<b>b</b>) NBR wear mechanism diagram under the influence of large size particles.</p>
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<p>Results of friction coefficient under different particle concentrations.</p>
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<p>Wear amount under the influence of particle concentration. (<b>a</b>) At particle size 5 μm, (<b>b</b>) at particle size 15 μm, (<b>c</b>) at particle size 25 μm, (<b>d</b>) at particle size 38 μm, (<b>e</b>) at particle size 45 μm, (<b>f</b>) at particle size 75 μm.</p>
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<p>Wear surface morphology under the influence of particle concentration. (<b>a</b>) At 1.5% sediment concentration, (<b>b</b>) at 3% sediment concentration, (<b>c</b>) at 4.5% sediment concentration, (<b>d</b>) at 6% sediment concentration, (<b>e</b>) at 7.5% sediment concentration, (<b>f</b>) at 9% sediment concentration.</p>
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<p>Wear mechanism in a small-sized particles environment with different sediment concentrations. (<b>a</b>) Low concentration. (<b>b</b>) medium concentration. (<b>c</b>) high concentration.</p>
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<p>Wear mechanism in a large-sized particles environment with different sediment concentrations. (<b>a</b>) Low concentration. (<b>b</b>) medium concentration. (<b>c</b>) high concentration.</p>
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<p>Schematic diagram of the synergistic mechanism. (<b>a</b>) Rolling wear model, (<b>b</b>) micro-cutting and rolling wear model.</p>
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10 pages, 3849 KiB  
Communication
Tunable Single-Longitudinal-Mode Thulium–Holmium Co-Doped Fiber Laser with an Ultra-Narrow Linewidth by Utilizing a Triple-Ring Passive Sub-Ring Resonator
by Pengfei Wang, Fengping Yan, Qi Qin, Dandan Yang, Ting Feng, Peng Liu, Ting Li, Chenhao Yu, Xiangdong Wang, Hao Guo, Yuezhi Cai, Wenjie Ji and Youchao Jiang
Photonics 2025, 12(1), 19; https://doi.org/10.3390/photonics12010019 - 28 Dec 2024
Viewed by 333
Abstract
A low-cost, wavelength-tunable single-longitudinal-mode (SLM) thulium–holmium co-doped fiber laser (THDFL) in a 2 μm band with a simple structure is described in the present paper. To obtain a stable SLM and narrow laser linewidth, a five-coupler-based three-ring (FCTR) filter is utilized in the [...] Read more.
A low-cost, wavelength-tunable single-longitudinal-mode (SLM) thulium–holmium co-doped fiber laser (THDFL) in a 2 μm band with a simple structure is described in the present paper. To obtain a stable SLM and narrow laser linewidth, a five-coupler-based three-ring (FCTR) filter is utilized in the ring cavity of the fiber laser. Tunable SLM wavelength output from THDFLs with kHz linewidths can be achieved by designing the FCTR filter with an effective free-spectral range and a 3 dB bandwidth at the main resonant peak. The measurement results show that the laser is in the SLM lasing state, with a highly stabilized optical spectrum, a linewidth of approximately 9.45 kHz, an optical signal-to-noise ratio as high as 73.6 dB, and a relative intensity noise of less than −142.66 dB/Hz. Furthermore, the wavelength can be tuned in the range of 2.6 nm. The proposed fiber laser has a wide range of applications, including coherence optical communication, optical fiber sensing, and dense wavelength-division-multiplexing. Full article
(This article belongs to the Special Issue Advanced Fiber Laser Technology and Its Application)
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<p>(<b>a</b>) Experimental configuration of THDFL. LD: laser diode; WDM: wavelength division multiplexer; THDF: thulium–holmium co-doped fiber; CIR: circulator; FBG: fiber Bragg grating; OC: optical coupler; (<b>b</b>) schematic diagram of the proposed FCTR filter; (<b>c</b>) transmission and reflection spectra of the FBG.</p>
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<p>Signal-flow graph representation of the sub-ring cavity.</p>
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<p>Simulated spectra of the proposed FCTR filter. The inset is a zoom-in of the main resonant peak of the FCTR filter.</p>
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<p>(<b>a</b>) Spectrum of the single-wavelength at 2048.39 nm; (<b>b</b>) fluctuations in wavelength and power at 2048.39 nm.</p>
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<p>(<b>a</b>) The self-homodyne RF spectrum measured using a signal analyzer with a range of 0–100 MHz; (<b>b</b>) 0–500 MHz; and (<b>c</b>) 0–1000 MHz; (<b>d</b>) the spectrum of the main cavity without an FCTR filter.</p>
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<p>RIN spectra of the proposed SLM THDFL, in 0–5 MHz, using a RBW of 10 kHz for the signal analyzer. Insets show the same measurements in the 0–200 kHz range using a RBW of 100 Hz with relaxation oscillation peaks.</p>
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<p>Frequency noise PSD of the constructed SLM THDFL, and the linewidths at different integration times.</p>
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<p>The spectrum of the THDFL with a tunable wavelength range of ~2.6 nm.</p>
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17 pages, 4791 KiB  
Article
Photoreconfigurable Metasurface for Independent Full-Space Control of Terahertz Waves
by Zhengxuan Jiang, Guowen Ding, Xinyao Luo and Shenyun Wang
Sensors 2025, 25(1), 119; https://doi.org/10.3390/s25010119 - 27 Dec 2024
Viewed by 497
Abstract
We present a novel photoreconfigurable metasurface designed for independent and efficient control of electromagnetic waves with identical incident polarization and frequency across the entire spatial domain. The proposed metasurface features a three-layer architecture: a top layer incorporating a gold circular split ring resonator [...] Read more.
We present a novel photoreconfigurable metasurface designed for independent and efficient control of electromagnetic waves with identical incident polarization and frequency across the entire spatial domain. The proposed metasurface features a three-layer architecture: a top layer incorporating a gold circular split ring resonator (CSRR) filled with perovskite material and dual C-shaped perovskite resonators; a middle layer of polyimide dielectric; and a bottom layer comprising a perovskite substrate with an oppositely oriented circular split ring resonator filled with gold. By modulating the intensity of a laser beam, we achieve autonomous manipulation of incident circularly polarized terahertz waves in both transmission and reflection modes. Simulation results demonstrate that the metasurface achieves a cross-polarized transmission coefficient of 0.82 without laser illumination and a co-polarization reflection coefficient of 0.8 under laser illumination. Leveraging the geometric phase principle, adjustments to the rotational orientation of the reverse split ring and dual C-shaped perovskite structures enable independent control of transmission and reflection phases. Furthermore, the proposed metasurface induces a +1 order orbital angular momentum in transmission and +2 order in reflection, facilitating beam deflection through metasurface convolution principles. Imaging using metasurface digital imaging technology showcases patterns “NUIST” in reflection and “LOONG” in transmission, illustrating the metasurface design principles via the proposed metasurface. The proposed metasurface’s capability for full-space control and reconfigurability presents promising applications in advanced imaging systems, dynamic beam steering, and tunable terahertz devices, highlighting its potential for future technological advancements. Full article
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<p>(<b>a</b>) OAM Mode 1 in transmission mode under high laser beam illumination for Metasurface I. (<b>b</b>) OAM Mode 2 in reflection mode without laser beam illumination for Metasurface I. (<b>c</b>) Holographic imaging with high laser beam illumination, generating a holographic image of the letters “NUIST” in reflection mode for Metasurface II. (<b>d</b>) Holographic imaging without laser beam illumination, generating a holographic image of the letters “LOONG” in transmission mode for Metasurface II.</p>
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<p>(<b>a</b>) Schematic of the proposed three-layer metasurface. (<b>b</b>) Top layer with CSRR and dual <span class="html-italic">C</span>-shaped resonators. (<b>c</b>) Bottom layer with circular split ring resonator.</p>
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<p>(<b>a</b>) Phase of co-polarized reflection coefficients (<span class="html-italic">r<sub>xx</sub></span> and <span class="html-italic">r<sub>yy</sub></span>) and co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) under laser beam illumination. (<b>b</b>) Phase of co-polarized reflection coefficients (<span class="html-italic">r<sub>xx</sub></span> and <span class="html-italic">r<sub>yy</sub></span>) and co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) without laser beam illumination. (<b>c</b>) Amplitude of co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) and co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) under laser beam illumination. (<b>d</b>) Amplitude of co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) and co-polarized transmission coefficients (<span class="html-italic">t<sub>xx</sub></span> and <span class="html-italic">t<sub>yy</sub></span>) without laser beam illumination.</p>
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<p>(<b>a</b>) Reflection amplitude and transmission amplitude at different rotation angles when unit is under laser beam illumination. (<b>b</b>) Transmission amplitude and reflection amplitude at different rotation angles when unit is without laser beam illumination. (<b>c</b>) Reflection phase at different rotation angles when unit is under laser beam illumination. (<b>d</b>) Transmission phase at different rotation angles when unit is without laser beam illumination.</p>
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<p>(<b>a</b>) Surface current distribution on the top layer under strong laser beam illumination, showing time-varying current distribution within the period. (<b>b</b>) Surface current distribution on the bottom layer under strong laser beam illumination, showing time-varying current distribution within the period. (<b>c</b>) Surface current distribution on the top layer without laser beam illumination, showing time-varying current distribution within the period. (<b>d</b>) Surface current distribution on the bottom layer without laser beam illumination, showing time-varying current distribution within the period.</p>
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<p>(<b>a</b>) Phase gradients along the +<span class="html-italic">x</span> direction. (<b>b</b>) Phase gradients along the −<span class="html-italic">x</span> direction. (<b>c</b>) Far-field distribution of a +1 order vortex beam deflected by 30° in the +<span class="html-italic">x</span> direction under strong laser beam illumination. (<b>d</b>) Far-field distribution of a −2 order vortex beam deflected by 30° in the −<span class="html-italic">x</span> direction without laser beam illumination. (<b>e</b>) Planar electric field intensity and phase distribution of the +1 order vortex beam under strong laser beam illumination, perpendicular to the 30° direction. (<b>f</b>) Planar electric field intensity and phase distribution of the −2 order vortex beam without laser beam illumination, perpendicular to the −30° direction.</p>
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<p>(<b>a</b>) Target images: “Zhu” in reflection mode, “Long” in transmission mode. (<b>b</b>) Phase distribution for holographic images, with phase changes from 0° to 360°. (<b>c</b>) Metasurface design layout with 50 × 50 unit structures in top and bottom layers. (<b>d</b>) Simulation results under different laser beam illumination: “Zhu” in reflection mode under laser beam illumination; “Long” in transmission mode without laser beam illumination.</p>
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<p>(<b>a</b>) Target images in reflection mode. (<b>b</b>) Phase distribution for reflection mode calculated using the GS algorithm. (<b>c</b>) Reproduced image of “NUIST” in reflection mode. (<b>d</b>) Target images in transmission mode. (<b>e</b>) Phase distribution for transmission mode calculated using the GS algorithm. (<b>f</b>) Reproduced image of “LOOGN” in transmission mode.</p>
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<p>(<b>a</b>) Near-field imaging results. (<b>b</b>) Far-field electric field distribution in reflection mode. (<b>c</b>) Far-field electric field distribution in transmission mode.</p>
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21 pages, 7222 KiB  
Article
Design of Multi-Time Programmable Intellectual Property with Built-In Error Correction Code Function Based on Bipolar–CMOS–DMOS Process
by Longhua Li, Soonwoo Kwon, Dohoon Kim, Dongseob Kim, Panbong Ha, Doojin Lee and Younghee Kim
Electronics 2025, 14(1), 68; https://doi.org/10.3390/electronics14010068 - 27 Dec 2024
Viewed by 573
Abstract
The coupling capacitor of the MTP cell used in this paper is an NCAP-type capacitor that has only a source contact, and the layout size of the unit cell is 6.184 μm × 6.295 μm (=38.93 μm2), which is 0.44% smaller [...] Read more.
The coupling capacitor of the MTP cell used in this paper is an NCAP-type capacitor that has only a source contact, and the layout size of the unit cell is 6.184 μm × 6.295 μm (=38.93 μm2), which is 0.44% smaller than the MTP cell that uses the coupling capacitor of the conventional NMOS transistor type that has both a source contact and a drain contact. In addition, a 4 Kb MTP IP with a built-in ECC function using an extended Hamming code capable of single-error correction and double-error detection was designed for safety considerations. In this paper, a new test algorithm is proposed to test whether the ECC function operates normally in the MTP IP with a built-in ECC function, and it is confirmed through a test using logic tester equipment that the output data DOUT[7:0] and the error flag ERROR_FLAG[1:0] are exactly the same in the cases of no error, a single-bit error, and a double-bit error. In addition, by sharing a current-controlled ring oscillator circuit that uses a current-starved inverter in the VPP, VNN, and VNNL charge pumping circuits that share a single ring oscillator in the erase and program operation modes of the MTP IP and using the regulated VPVR as power, the pumping capacitor size is reduced, and a new technology to reduce ripple voltage variation is proposed. Meanwhile, in the VNN level detector circuit that detects whether the VNN has reached the target voltage, a folded-cascode CMOS OP-AMP whose output swing voltage is almost VDD is used instead of a differential amplifier circuit with a PMOS differential input pair to ensure that normal VNN level detection operation occurs. Full article
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<p>The MTP cell circuit used [<a href="#B14-electronics-14-00068" class="html-bibr">14</a>].</p>
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<p>MTP cell using a coupling capacitor in the form of an NMOS transistor: (<b>a</b>) process cross-section and (<b>b</b>) layout image [<a href="#B14-electronics-14-00068" class="html-bibr">14</a>].</p>
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<p>MTP cell using NCAP-type coupling capacitor: (<b>a</b>) process cross-section and (<b>b</b>) layout image.</p>
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<p>Block diagram of 4 Kb MTP IP with built-in ECC function using (13, 8) extended Hamming code.</p>
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<p>Boolean functions that generate the 5-bit parity bits.</p>
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<p>Boolean functions that generate 4-bit syndromes.</p>
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<p>Error correction process.</p>
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<p>Boolean functions for correcting single errors using syndrome bits.</p>
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<p>Boolean functions of odd parity bit for double-error detection.</p>
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<p>Timing diagram for ECC function test mode for single-error detection.</p>
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<p>Timing diagram for ECC function test mode for double-error detection.</p>
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<p>Ring oscillator circuits using voltage regulation voltage as power: (<b>a</b>) circuit using a conventional CMOS inverter and (<b>b</b>) circuit using the proposed current-starved CMOS inverter.</p>
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<p>Block diagram of a charge pump circuit that uses the output voltage of the newly proposed voltage regulator as power and uses a shared current-starved ring oscillator.</p>
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<p>VNN level detector circuit.</p>
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<p>Comparator circuits used in the VNN level detector circuit: (<b>a</b>) using a differential amplifier and (<b>b</b>) using a folded-cascode CMOS OP-AMP.</p>
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<p>Layout image of the designed 4 Kb MTP memory IP.</p>
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<p>VTC measurement results from the MTP cells depicted in <a href="#electronics-14-00068-f003" class="html-fig">Figure 3</a> for data memory and parity memory in the MTP IP with a built-in ECC function: (<b>a</b>) data memory and (<b>b</b>) parity memory.</p>
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16 pages, 5129 KiB  
Article
Detection of Human Bladder Epithelial Cancerous Cells with Atomic Force Microscopy and Machine Learning
by Mikhail Petrov, Nadezhda Makarova, Amir Monemian, Jean Pham, Małgorzata Lekka and Igor Sokolov
Cells 2025, 14(1), 14; https://doi.org/10.3390/cells14010014 - 26 Dec 2024
Viewed by 418
Abstract
The development of noninvasive methods for bladder cancer identification remains a critical clinical need. Recent studies have shown that atomic force microscopy (AFM), combined with pattern recognition machine learning, can detect bladder cancer by analyzing cells extracted from urine. However, these promising findings [...] Read more.
The development of noninvasive methods for bladder cancer identification remains a critical clinical need. Recent studies have shown that atomic force microscopy (AFM), combined with pattern recognition machine learning, can detect bladder cancer by analyzing cells extracted from urine. However, these promising findings were limited by a relatively small patient cohort, resulting in modest statistical significance. In this study, we corroborated the AFM technique’s capability to identify bladder cancer cells with high accuracy using a controlled model system of genetically purified human bladder epithelial cell lines, comparing cancerous cells with nonmalignant controls. By processing AFM adhesion maps through machine learning algorithms, following previously established methods, we achieved an area under the ROC curve (AUC) of 0.97, with 91% accuracy in cancer cell identification. Furthermore, we enhanced cancer detection by incorporating multiple imaging channels recorded with AFM operating in Ringing mode, achieving an AUC of 0.99 and 93% accuracy. These results demonstrated strong statistical significance (p < 0.0001) in this well-defined model system. While this controlled study does not capture the biological variation present in clinical settings, it provides independent support for AFM-based detection methods and establishes a rigorous technical foundation for further clinical development of AFM imaging-based methods for bladder cancer detection. Full article
(This article belongs to the Special Issue Advances in Scanning Probe Microscopy in Cell Biology)
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<p>Representative examples of HCV29 and TCCSUP cells. (<b>a</b>) Optical images of the cells; the scale bar is 100 µm (one can also see a triangle shadow of the AFM cantilever). Shown are 10 × 10 µm<sup>2</sup> AFM images recorded in five channels used for the cell classification. (<b>b</b>) Height (Nanoscope channel), (<b>c</b>) adhesion (Nanoscope channel), (<b>d</b>) restored adhesion (ringing mode channel), (<b>e</b>) neck size (ringing mode channel), (<b>f</b>) disconnection distance (ringing mode channel).</p>
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<p>Ranking of surface parameters by Gini importance index. The height (Nanoscope channel), adhesion (Nanoscope channel), restored adhesion (ringing mode channel), neck size (ringing mode channel), and disconnection distance (ringing mode channel) channels, as well as the combined channels, are shown.</p>
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<p>ROC curves described in the classification of nonmalignant and cancerous cells when using the height (Nanoscope channel), adhesion (Nanoscope channel), restored adhesion (ringing mode channel), neck size (ringing mode channel), and disconnection distance (ringing mode channel) channels, as well as the combined channels.</p>
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<p>Multiple ROC curves and histograms of the AUCs obtained when the ML algorithm was developed on and applied to the data set with randomly assigned class to each cell. “No Classification” lines are drawn in the graphs showing ROC curves.</p>
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<p>Graphical description of the ringing mode channels used in this work. (<b>a</b>) Trajectory of the AFM probe scanning in subresonance tapping. (<b>b</b>) Graphical presentation of the neck size and disconnection distance channels. (<b>c</b>) Explanation of the restored adhesion.</p>
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23 pages, 5622 KiB  
Article
Power Flow Analysis of Ring AC/DC Hybrid Network with Multiple Power Electronic Transformers Based on Hybrid Alternating Iteration Power Flow Algorithm
by Zhen Zheng, Chenhong Huang, Xiaoli Ma, Wenwen Chen, Yinan Huang, Min Wang and Dongqian Pan
Processes 2025, 13(1), 7; https://doi.org/10.3390/pr13010007 - 24 Dec 2024
Viewed by 271
Abstract
AC/DC hybrid distribution networks with power electronic transformers (PETs) as distribution hubs are in line with the future development direction of the AC/DC hybrid distribution network. Unlike traditional transformers, power electronic transformers introduce new node types and may transform the network topology from [...] Read more.
AC/DC hybrid distribution networks with power electronic transformers (PETs) as distribution hubs are in line with the future development direction of the AC/DC hybrid distribution network. Unlike traditional transformers, power electronic transformers introduce new node types and may transform the network topology from radial to ring structures. These changes render traditional power flow calculation methods inadequate for achieving satisfactory results in AC/DC hybrid networks. In addition, existing commercial power flow calculation software packages are mainly based on the traditional AC power flow calculation method, which have limited support for the DC network. Especially when the DC network is coupled with the AC network, it is difficult to achieve a unified calculation of its power flow. To address these challenges, this paper proposes a novel power flow calculation method for ring AC/DC hybrid distribution networks with power electronic transformers. The proposed method is based on the alternating iterative method to ensure compatibility with mature AC power flow calculation programs in commercial software, thereby improving the feasibility of engineering applications. Firstly, the steady-state power flow calculation model of PET is constructed by analyzing that the working principle and control modes of power electronic transformer are proposed based on the source-load attributes of its connected subnetworks. According to the characteristics of the power electronic transformer, AC distribution network, and DC distribution network, a hybrid alternating iteration method combining the high computational accuracy of the Newton–Raphson (NR) method with the high efficiency of the Zbus Gaussian method in dealing with ring networks is proposed. On this basis, the power flow calculation model of the AC/DC hybrid distribution network with power electronic transformers is established. Finally, the simulation of the constructed 44-node ring AC/DC hybrid distribution network example is carried out. The simulation results show that the proposed method can not only converge reliably when the convergence accuracy is 1 × 10−6 p.u., but also ensure that the voltage magnitudes of all nodes are above 0.96 p.u. whose maximum offset value is 0.789% when the outputs of the connected distributed generations fluctuate, which verifies the effectiveness and accuracy of the proposed method. Full article
(This article belongs to the Section Energy Systems)
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<p>Traditional AC distribution networks without DC bus.</p>
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<p>AC/DC hybrid distribution networks with non-isolated bidirectional converters.</p>
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<p>AC/DC hybrid distribution networks with PETs.</p>
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<p>Physical structure of PET.</p>
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<p>Model of the AC port based on VSC.</p>
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<p>Model of the DC port based on the DC/DC converter.</p>
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<p>A flowchart of the power flow calculation process for AC/DC hybrid distribution networks with PETs.</p>
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<p>Improved IEEE 33-bus system connected to the DC system.</p>
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<p>Partition results.</p>
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<p>Active power of all ports of two PETs.</p>
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<p>Voltage magnitude of all ports of two PETs.</p>
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<p>Modulation ratio of AC ports of two PETs.</p>
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<p>Outputs of PVs and WTs in three cases.</p>
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<p>Comparisons of the bus voltage magnitudes between three cases.</p>
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<p>Bus voltage offset distribution of case 2 and case 3.</p>
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<p>Comparisons of the active power of all ports of two PETs between three cases.</p>
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18 pages, 9706 KiB  
Article
Dynamics Study of Hybrid Support Flywheel Energy Storage System with Damping Ring Device
by Mingming Hu, Kun Liu, Jingbo Wei, Eryong Hou, Duhe Liu and Xi Zhao
Actuators 2024, 13(12), 532; https://doi.org/10.3390/act13120532 - 23 Dec 2024
Viewed by 343
Abstract
The flywheel energy storage system (FESS) of a mechanical bearing is utilized in electric vehicles, railways, power grid frequency modulation, due to its high instantaneous power and fast response. However, the lifetime of FESS is limited because of significant frictional losses in mechanical [...] Read more.
The flywheel energy storage system (FESS) of a mechanical bearing is utilized in electric vehicles, railways, power grid frequency modulation, due to its high instantaneous power and fast response. However, the lifetime of FESS is limited because of significant frictional losses in mechanical bearings and challenges associated with passing the critical speed. To suppress the unbalanced response of FESS at critical speed, a damping ring (DR) device is designed for a hybrid supported FESS with mechanical bearing and axial active magnetic bearing (AMB). Initially, the dynamic model of the FESS with DR is established using Lagrange’s equation. Moreover, the dynamic parameters of the DR are obtained by experimental measurements using the method of free vibration attenuation. Finally, the influence of the DR device on the critical speed and unbalanced response of FESS is analyzed. The results show that the designed DR device can effectively reduce the critical speed of FESS, and increase the first and second mode damping ratio. The critical speed is reduced from 13,860 rpm to 5280 rpm. Compared with FESS of the mechanical bearing, the unbalanced response amplitude of the FESS with DR is reduced by more than 87.8%, offering promising technical support for the design of active and passive control systems in FESS. Full article
(This article belongs to the Special Issue Actuator Technology for Active Noise and Vibration Control)
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<p>Schematic of FESS structure.</p>
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<p>Simplified model of FESS rotor–bearing system.</p>
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<p>FESS.</p>
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<p>Unfilled DR.</p>
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<p>Cross-section of the DR measuring device.</p>
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<p>Experimental procedure of DR.</p>
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<p>Experimental platform of DR.</p>
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<p>Curve fitting of free decay data.</p>
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<p>Modal shapes of FESS with DR at 0 rpm: (<b>a</b>) first modal, (<b>b</b>) second modal, (<b>c</b>) third modal, (<b>d</b>) fourth modal.</p>
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<p>Modal shapes of FESS with DR at 12,000 rpm: (<b>a</b>) first modal, (<b>b</b>) second modal, (<b>c</b>) third modal, (<b>d</b>) fourth modal.</p>
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<p>Variation of 1st- to 4th-order modal damping ratio with damping coefficients: (<b>a</b>) <math display="inline"><semantics> <msub> <mi>c</mi> <mn>1</mn> </msub> </semantics></math>, (<b>b</b>) <math display="inline"><semantics> <msub> <mi>c</mi> <mn>4</mn> </msub> </semantics></math>.</p>
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<p>Campbell diagram of the FESS: (<b>a</b>) REB + DR, (<b>b</b>) REB.</p>
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<p>Variation of unbalanced response with stiffness: (<b>a</b>) upper bearing, (<b>b</b>) upper end face of flywheel.</p>
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<p>Variation of unbalanced response with damping: (<b>a</b>) upper bearing, (<b>b</b>) upper end face of flywheel.</p>
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<p>Comparison of unbalanced response: (<b>a</b>) upper bearing, (<b>b</b>) upper flywheel end face, (<b>c</b>) lower flywheel end face, (<b>d</b>) lower bearing.</p>
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17 pages, 8947 KiB  
Article
Exploring the Effect of Interface Contact States on Brush/Ring Current-Carrying Friction
by Chenshi Li, Xinze Zhao, Yaru Lv, Yang Li, Wanting Li and Wei Yang
Lubricants 2024, 12(12), 461; https://doi.org/10.3390/lubricants12120461 - 20 Dec 2024
Viewed by 452
Abstract
A carbon brush/collector ring set will have phenomena such as firing and ablation during operation, which is due to the existence of various abnormal contact modes of the brush/ring during operation, thus changing the carbon brush/collector ring interface state. To analyze the effects [...] Read more.
A carbon brush/collector ring set will have phenomena such as firing and ablation during operation, which is due to the existence of various abnormal contact modes of the brush/ring during operation, thus changing the carbon brush/collector ring interface state. To analyze the effects of different contact modes on the performance of the brush/ring, in this paper, we construct the contact modes of the air gap (loss of contact leads to the existence of a small gap between the two surfaces), direct contact (contact with abrasive particulate media), and surface porosity contact (contact when there is a large pit on the surface of the collector ring due to manufacturing quality defects and abnormal abrasion), and analyze the effects of the various states on the core parameters such as current conduction, ring surface damage, and carbon brush abrasion, which provide a basis for the active suppression of the damage. Full article
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<p>Brush/ring contact state during actual operation: (<b>a</b>) normal operation of collector ring; (<b>b</b>) air-gap contact state; (<b>c</b>) carbon powder impurity contact state; (<b>d</b>) collector ring surface pore contact.</p>
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<p>Surface roughness of collector ring.</p>
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<p>Carbon powder-coating production process.</p>
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<p>Toner coverage area. (<b>a</b>) 25% coverage; (<b>b</b>) 25% coverage; (<b>c</b>) 25% coverage; (<b>d</b>) 25% coverage.</p>
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<p>Pore arrangement. (<b>a</b>) 36°; (<b>b</b>) 45°; (<b>c</b>) 60°; (<b>d</b>) 90°.</p>
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<p>Experimental setup: (<b>a</b>) current-carrying friction and wear tester; (<b>b</b>) test method of pin–disk contact; (<b>c</b>) physical drawing of current-carrying friction and wear tester; (<b>d</b>) schematic diagram of test setup.</p>
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<p>Air-gap test stand.</p>
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<p>Variation in spark power and temperature at different voltages and rotational speeds of positive pole: (<b>a</b>–<b>c</b>) temperature variation curves at 10–30 V; (<b>d</b>–<b>f</b>) arc power variation curves at 10–30 V; (<b>g</b>) average temperature variation curves; (<b>h</b>) average arc power variation curves.</p>
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<p>Temperature changes in the contact surface under different voltages of the positive electrode of the carbon brush: (<b>a</b>) 10 V; (<b>b</b>) 20 V; (<b>c</b>) 30 V; (I) 200 r/min; (II) 300 r/min; (III) 400 r/min.</p>
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<p>Variation in spark power and temperature at different rotational speeds of carbon brush negative electrode: (<b>a</b>–<b>c</b>) temperature variation curves at 10–30 V; (<b>d</b>–<b>f</b>) arc power variation curves at 10–30 V; (<b>g</b>) mean temperature variation curves; (<b>h</b>) mean arc power variation curves.</p>
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<p>Temperature change in contact surface at different voltages of carbon brush positive pole: (<b>a</b>) 10 V; (<b>b</b>) 20 V; (<b>c</b>) 30 V; (I) speed of 200 r/min; (II) speed of 300 r/min; (III) speed of 400 r/min.</p>
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<p>Ablation morphology of carbon brush positive collector ring surface: (<b>a</b>–<b>c</b>) 200 r–400 r at 10 V; (<b>d</b>–<b>f</b>) 200 r–400 r at 20 V; (<b>g</b>–<b>i</b>) 200 r–400 r at 30 V.</p>
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<p>Ablation morphology of carbon brush negative collector ring surface: (<b>a</b>–<b>c</b>) 200 r–400 r at 10 V; (<b>d</b>–<b>f</b>) 200 r–400 r at 20 V; (<b>g</b>–<b>i</b>) 200 r–400 r at 30 V.</p>
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<p>Morphology of carbon brushes of different polarities after ablation at same rotational speed: (<b>a</b>–<b>c</b>) ablation of positive carbon brushes at 10–30 V; (<b>d</b>–<b>f</b>) ablation of negative carbon brushes at 10–30 V.</p>
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<p>Arc morphology under different current-carrying polarity: (<b>a</b>) carbon brush connected to positive electrode; (<b>b</b>) carbon brush connected to negative electrode.</p>
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<p>Mechanism of arc generation under different polarity: (<b>a</b>) brush connected to negative pole; (<b>b</b>) brush connected to positive pole.</p>
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<p>Temperature and contact resistance variation with different toner coverage: (<b>a</b>) temperature variation curves; (<b>b</b>) average temperature variation; (<b>c</b>) dynamic contact resistance variation curves; (<b>d</b>) line graph of average contact resistance variation.</p>
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<p>Variation in brush/ring friction performance with different toner coverage: (<b>a</b>) dynamic friction coefficient variation curves; (<b>b</b>) average friction coefficient line plot.</p>
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<p>Temperature and contact resistance variation in pore brushes/rings with different arrangements: (<b>a</b>) temperature variation curve; (<b>b</b>) average temperature variation; (<b>c</b>) dynamic contact resistance variation curve; (<b>d</b>) line graph of average contact resistance variation.</p>
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<p>Variation in friction performance of different arrangements of pore brushes/rings: (<b>a</b>) dynamic friction coefficient variation curve; (<b>b</b>) line graph of wear rate.</p>
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16 pages, 10770 KiB  
Article
A Tunable and Switchable Multi-Wavelength Erbium-Doped Fiber Laser Based on a Curvature Mach–Zehnder Interferometer Filter Using Thin-Core Fiber
by Christian Perezcampos-Mayoral, Jaime Gutiérrez-Gutiérrez, José Luis Cano-Pérez, Marciano Vargas-Treviño, Lorenzo Tepech-Carrillo, Erick Israel Guerra-Hernández, Itandehui Belem Gallegos-Velasco, Pedro Antonio Hernández-Cruz, Eeduardo Pérez-Campos-Mayoral, Victor Hugo Ojeda-Meixueiro, Julián Moisés Estudillo-Ayala, Juan Manuel Sierra-Hernandez and Roberto Rojas-Laguna
Appl. Sci. 2024, 14(24), 11578; https://doi.org/10.3390/app142411578 - 11 Dec 2024
Viewed by 494
Abstract
We propose and demonstrate a tunable and switchable multi-wavelength fiber ring laser configuration based on a Mach–Zehnder interferometer (MZI) filter. The MZI was fabricated using a core-offset splicing technique, with a 2 cm piece of thin-core erbium-doped fiber (TCEDF), with a core diameter [...] Read more.
We propose and demonstrate a tunable and switchable multi-wavelength fiber ring laser configuration based on a Mach–Zehnder interferometer (MZI) filter. The MZI was fabricated using a core-offset splicing technique, with a 2 cm piece of thin-core erbium-doped fiber (TCEDF), with a core diameter of 2.90 µm, coupled in the central region of the MZI between two segments of single-mode fiber (SMF). By applying curvature to the MZI filter, we generated lasing single-, double-, triple-, and quadruple-emission lines with a curvature range from 2.3452 m−1 to 6.0495 m−1. A single-emission lasing line can be tuned from 1556.63 nm to 1564.25 nm with a tuning span of 7.62 nm and an SMSR of 49.80 dB. The laser emission can be switched to quadruple- and triple-emission lasing signals, with SMSR values of 39.96 dB and 36.83 dB, respectively. The dual-narrow emission lasing signal can be tuned from 1564.56 nm to 1561.34 nm, with an SMSR of 40.46 dB. Another lasing dual-emission signal can be tuned from 1585.69 nm to 1576.89 nm, producing an 8.8 nm tuning range, and from 1572.53 nm to 1563.66 nm, producing an 8.87 nm range, with the best SMSR of 42.35 dB. Full article
(This article belongs to the Special Issue Recent Trends in Fiber Optic Sensor: Technology and Applications)
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<p>Fiber clamping for SMF/TCEDF/SMF splices. (<b>a</b>) This demonstrates how to adhere the fiber to the metric rod with the masking tape and (<b>b</b>) illustrates how splicing is accomplished with the fusion splicer.</p>
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<p>Core-offset splice SMF/TCEDF/SMF design. (<b>a</b>) Illustrates the splicing between fibers, (<b>b</b>) shows the TCEDF cut, (<b>c</b>) U-shape of the MZI filter, (<b>d</b>) exhibits the z-side view of the MZI.</p>
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<p>(<b>a</b>) Interference spectra generated in the optical cavity of each MZI filter, (<b>b</b>) spatial frequency of the transmission spectrum generated by every filter.</p>
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<p>Diagram of the MTEFL ring array: (<b>a</b>) illustrates the configuration scheme, and (<b>b</b>) depicts the process for inducing curvature in the MZI filter to generate wavelength-switchable tunable emission lines.</p>
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<p>MTEFL emission tuning and switching cases generated for single (state-a), quadruple (state-b), triple (state-c), narrow-double (state-d), and double (state-e) lasing signals.</p>
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<p>(State-a) single-emission signal. (<b>a</b>) Tuning lines, (<b>b</b>) emission samples of curvature and SNR, (<b>c</b>) SMSR and SNR of the most significant peaks and their comparison, (<b>d</b>) the polynomial fit between the curvature data and its wavelength shift.</p>
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<p>Switch with quad-emission line. (<b>a</b>) SMSR on each peak, (<b>b</b>) power difference between the peaks and their separation.</p>
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<p>(State-c) double switch of triple-emission signals: (<b>a</b>) SMSR on the first switch, (<b>b</b>) separation and power of peaks, (<b>c</b>) SMSR of the second switch, (<b>d</b>) separation and the power of peaks.</p>
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<p>(State-c) double switch of triple-emission signals: (<b>a</b>) SMSR on the first switch, (<b>b</b>) separation and power of peaks, (<b>c</b>) SMSR of the second switch, (<b>d</b>) separation and the power of peaks.</p>
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<p>Narrow-dual-emission signals (state-d). (<b>a</b>) Tuning and the potential difference between peaks and their wavelength comparisons, (<b>b</b>) most significative peaks and power comparison, (<b>c</b>) sensitivity compared to the dispersion of curvature samples.</p>
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<p>Double-emission signal (state-e). (<b>a</b>) Tuning and most significant power peaks, (<b>b</b>) separation comparison, (<b>c</b>) peaks power comparison, (<b>d</b>) sensitivity generated with the curvature/wavelength samples.</p>
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<p>Double-emission signal (state-e). (<b>a</b>) Tuning and most significant power peaks, (<b>b</b>) separation comparison, (<b>c</b>) peaks power comparison, (<b>d</b>) sensitivity generated with the curvature/wavelength samples.</p>
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<p>(<b>a</b>) Stability test of the single initial and final emission, (<b>b</b>) power variation, (<b>c</b>) wavelength variation.</p>
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<p>First and last emissions signals of the dual-narrow lasing lines. (<b>a</b>) Stability test, (<b>b</b>) power fluctuation, (<b>c</b>) wavelength stability.</p>
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<p>Stability tests of the dual lasing lines. (<b>a</b>) Stability test on the first emission, (<b>b</b>) power fluctuation, (<b>c</b>) wavelength stability, (<b>a’</b>) stability test on the last emission, (<b>b’</b>) power fluctuation, (<b>c’</b>) wavelength stability.</p>
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<p>(<b>a</b>) Stability tests of the quad-emission line, (<b>b</b>) power variation, (<b>c</b>) wavelength variation.</p>
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<p>Stability tests of the triple emissions. (<b>a</b>) On the first switch, (<b>b</b>) power variation, (<b>c</b>) wavelength variation, (<b>a’</b>) test on the second switch, (<b>b’</b>) power variation, (<b>c’</b>) wavelength variation.</p>
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19 pages, 7237 KiB  
Article
Relationship Between Fracture Fractal and Mechanical Properties of 5083 Aluminum Alloy Sheet Prepared by Alternate Ring-Groove Pressing and Torsion
by Chunhui Zhang, Yu Wang, Mingxin Wang, Wenhao Li, Chunxiang Zhang and Junting Luo
Metals 2024, 14(12), 1382; https://doi.org/10.3390/met14121382 - 2 Dec 2024
Viewed by 539
Abstract
In this study, the tensile fracture morphology of a 5083 aluminum alloy sheet prepared by alternate ring-groove pressing torsion and torsional flattening at room temperature (ARPT-TF-R) under different numbers of torsional flattening passes was analyzed. The box dimension method was used to calculate [...] Read more.
In this study, the tensile fracture morphology of a 5083 aluminum alloy sheet prepared by alternate ring-groove pressing torsion and torsional flattening at room temperature (ARPT-TF-R) under different numbers of torsional flattening passes was analyzed. The box dimension method was used to calculate the fractal dimension, and formulas for the quantitative relationships between the tensile properties and Vickers hardness of 5083 aluminum alloy sheet under different process conditions and the fractal dimension were established. The results indicated that the fracture mode of the sheet prepared by one pass was microporous aggregation fracture, and the number of large-sized dimples was small. The plate prepared by two passes had a greater number of micropores, and the dimple size was relatively small. The fractal dimension of the aluminum alloy sheet prepared by ARPT-TF-R at room temperature was 1.77–1.84. As the number of torsional flattening passes increased, the yield strength, tensile strength, Vickers hardness, and fractal dimension of the aluminum alloy sheet increased. Full article
(This article belongs to the Special Issue Metal Plastic Deformation and Forming)
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<p>Metallographic structure of 5083 aluminum alloy original sheet: (<b>a</b>) are low-magnification images; (<b>b</b>) are high-magnification images.</p>
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<p>Waveform position relationship of two ring wave molds.</p>
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<p>Flowchart of severe plastic deformation in the ARPT-TF-R process. Reprinted from Ref. [<a href="#B19-metals-14-01382" class="html-bibr">19</a>]. (<b>a</b>–<b>f</b>) is the strengthening process of alternating pressing-torsion deformation and leveling of the plate through two sets of ring wave molds and torsion flat molds. 1—First ring wave mold die upper die; 2—First ring wave die lower die; 3—Twist flat die upper die; 4—Twist flat lower die; 5—Second ring wave die upper die; 6—Second ring wave die lower die.</p>
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<p>Metallographic structure of ring wave repeated compression torsion–room temperature torsion flat treatment plate: (<b>a</b>) One-pass processing; (<b>b</b>) two-pass processing.</p>
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<p>SEM micro-morphology of tensile fracture of sheet processed by one pass of torsional flattening at room temperature: (<b>a</b>,<b>b</b>) are low-magnification images, and (<b>c</b>,<b>d</b>) are high-magnification images.</p>
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<p>SEM micro-morphology of tensile fracture of sheet processed by two pass of torsional flattening at room temperature: (<b>a</b>,<b>b</b>) are low-magnification images, and (<b>c</b>,<b>d</b>) are high-magnification images.</p>
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<p>Pretreatment and fitting plot of tensile fracture morphology of the original sheet at room temperature: (<b>a</b>) original; (<b>b</b>) grayscale adjustment; (<b>c</b>) histogram equalization; (<b>d</b>) binarization; (<b>e</b>) fitting plot.</p>
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<p>Pretreatment of low-magnification fracture morphology and fitting curve of sheet processed by one-pass torsional flattening at room temperature: (<b>a</b>) original picture; (<b>b</b>) grayscale adjustment; (<b>c</b>) histogram equalization; (<b>d</b>) binarization; and (<b>e</b>) fitting curve.</p>
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<p>Pretreatment of high-magnification tensile fracture morphology and fitting curve of sheet processed by one-pass torsional flattening at room temperature: (<b>a</b>) original picture; (<b>b</b>) grayscale adjustment; (<b>c</b>) histogram equalization; (<b>d</b>) binarization; and (<b>e</b>) fitting curve.</p>
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<p>Pretreatment of low-magnification tensile fracture morphology and fitting curve of sheet processed by two-pass torsional flattening at room temperature: (<b>a</b>) original picture; (<b>b</b>) grayscale adjustment; (<b>c</b>) histogram equalization; (<b>d</b>) binarization; and (<b>e</b>) fitting curve.</p>
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<p>Pretreatment of high-magnification tensile fracture morphology and fitting curve of sheet processed by torsional flattening at room temperature: (<b>a</b>) original picture; (<b>b</b>) grayscale adjustment; (<b>c</b>) histogram equalization; (<b>d</b>) binarization; and (<b>e</b>) fitting curve.</p>
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<p>Stress-strain curve of sheet processed by ARPT-TF-R.</p>
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<p>Fitting curve of the relationship between tensile elongation and fractal dimension of sheet processed by torsional flattening at room temperature: (<b>a</b>) yield strength; (<b>b</b>) tensile strength; and (<b>c</b>) elongation.</p>
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<p>Comparison of hardnesses between original sheet and sheet subjected to ARPT-TF-R.</p>
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<p>Fitting curve of relationship between hardness and fractal dimension of sheet subjected to torsional flattening at room temperature.</p>
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11 pages, 12766 KiB  
Communication
Few-Mode Fiber with Low Spontaneous Raman Scattering for Quantum Key Distribution and Classical Optical Communication Coexistence Systems
by Qi Zhao, Jianjun Tang, Weiwen Kong, Zhenyu Zhao, Jingjing Zheng and Yang Liu
Sensors 2024, 24(23), 7645; https://doi.org/10.3390/s24237645 - 29 Nov 2024
Viewed by 462
Abstract
In this paper, the theoretical model of spontaneous Raman scattering (SpRS) in few-mode fiber (FMF) is discussed. The influence of SpRS on quantum key distribution (QKD) in FMF is evaluated by combining wavelength division multiplexing (WDM) and space division multiplexing (SDM) techniques. On [...] Read more.
In this paper, the theoretical model of spontaneous Raman scattering (SpRS) in few-mode fiber (FMF) is discussed. The influence of SpRS on quantum key distribution (QKD) in FMF is evaluated by combining wavelength division multiplexing (WDM) and space division multiplexing (SDM) techniques. On this basis, an improved ring-assisted FMF is designed and characterized; the transmission distance can be increased by up to 54.5% when choosing different multi-channels. The effects of forward and backward SpRS on QKD are also discussed. Full article
(This article belongs to the Special Issue Challenges and Future Trends in Optical Communications)
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<p>The radius and refractive index distribution of (<b>a</b>) step-index fiber and (<b>b</b>) ring-core fiber (RCF). (<b>c</b>) The modes that can be supported in fibers.</p>
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<p>The relationship between secure key rate (SKR) and transmission distance in SMF.</p>
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<p>The relationship between SKR and transmission distance for classical signals in single mode. (<b>a</b>) FMF<sub>1</sub>, (<b>b</b>) FMF<sub>2</sub>, (<b>c</b>) RCF, and (<b>d</b>) 6MF.</p>
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<p>The relationship between SKR and transmission distance for classical signals in multiple modes. (<b>a</b>) FMF<sub>1</sub>, (<b>b</b>) FMF<sub>2</sub>, (<b>c</b>) RCF, and (<b>d</b>) 6MF.</p>
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<p>The relationship between SKR and transmission distance for classical signals in multiple modes. (<b>a</b>) FMF<sub>1</sub>, (<b>b</b>) FMF<sub>2</sub>, (<b>c</b>) RCF, and (<b>d</b>) 6MF.</p>
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<p>The radius and refractive index distribution of the ring-assisted FMF.</p>
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<p>(<b>a</b>) The variation in Δ<span class="html-italic">n<sub>eff</sub></span> with <span class="html-italic">a<sub>co</sub></span><sub>1</sub> and <span class="html-italic">a<sub>co</sub></span><sub>2</sub>. (<b>b</b>) The variation in Δ<span class="html-italic">n<sub>eff</sub></span> with <span class="html-italic">n<sub>co</sub></span><sub>2</sub> and <span class="html-italic">n<sub>co</sub></span><sub>3</sub>.</p>
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<p>The relationship between SKR and transmission distance when using ring-assisted FMF (solid line) and FMF<sub>2</sub> (dashed line) with four wavelengths in each mode. Among them, the classical channel is (<b>a</b>) one mode and (<b>b</b>) multiple modes.</p>
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<p>The relationship between SKR and transmission distance when using ring-assisted FMF (solid line) and FMF<sub>2</sub> (dashed line) with ten wavelengths in each mode. Among them, the classical channel is (<b>a</b>) one mode; (<b>b</b>) multiple modes.</p>
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<p>The relationship between SKR and transmission distance when using ring-assisted FMF with (<b>a</b>) four wavelengths and (<b>b</b>) ten wavelengths in each mode.</p>
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14 pages, 5075 KiB  
Article
Multimode Miniature Polarization-Sensitive Metamaterial Absorber with Ultra-Wide Bandwidth in the K Band
by Zhonghang Ji, Yida Song, Mandi Gao, Qiong Zhang and Yunqing Liu
Micromachines 2024, 15(12), 1446; https://doi.org/10.3390/mi15121446 - 29 Nov 2024
Viewed by 569
Abstract
Metamaterial absorbers have gained widespread applications in fields such as sensing, imaging, and electromagnetic cloaking due to their unique absorption characteristics. This paper presents the design and fabrication of a novel K-band polarization-sensitive metamaterial absorber, which operates in the frequency range of 20.76 [...] Read more.
Metamaterial absorbers have gained widespread applications in fields such as sensing, imaging, and electromagnetic cloaking due to their unique absorption characteristics. This paper presents the design and fabrication of a novel K-band polarization-sensitive metamaterial absorber, which operates in the frequency range of 20.76 to 24.20 GHz for both TE and TM modes, achieving an absorption rate exceeding 90% and a bandwidth of up to 3.44 GHz. The structure of the metamaterial absorber consists of a rectangular aperture metallic patch, two metallic rings, and two metallic strips, with a metallic patch structure on the back. Both metallic patches are printed on a 1.575 mm-thick FR-4 substrate. In the TE mode, the performance shows diagonal symmetry, with a minimum absorption bandwidth of 1.4 GHz at 45° and a maximum of 3.44 GHz at 0°. The absorption rate exceeds 90% across various polarization angles. In terms of conventional modes, both the TE and TM modes can achieve ultra-wideband absorption. For specific scenarios requiring single-frequency or multi-frequency absorption, the desired functionality can be realized by varying the incident angle. These exceptional characteristics confer strong applicability for high-bandwidth electromagnetic wave absorption and specific frequency point absorption, indicating significant potential and practical value in the field of wireless communication. Full article
(This article belongs to the Special Issue Functional Materials and Microdevices)
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<p>(<b>a</b>) Front view of the metamaterial. (<b>b</b>) Side view of the metamaterial.</p>
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<p>(<b>a</b>) Steps for absorber design. (<b>b</b>) Absorption rate curves for each step. (<b>c</b>) <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mrow> <mn>11</mn> </mrow> </msub> </mrow> </semantics></math> curves for each step.</p>
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<p>(<b>a</b>) Equivalent circuit diagram. (<b>b</b>) Comparison of ADS and CST simulation results.</p>
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<p>The effective parameters of the metamaterials in the frequency range of 18 GHz to 26 GHz. The blue dashed line represents the real part, and the black dashed line represents the imaginary part. (<b>a</b>) Normalized impedance. (<b>b</b>) Permeability. (<b>c</b>) Refractive index. (<b>d</b>) Permittivity.</p>
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<p>An illustration of the real parts of the permittivity and permeability in the frequency range of 18 GHz to 26 GHz. The black dot–dash line represents the real part of the permittivity, and the blue line represents the real part of the permeability.</p>
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<p>From left to right are the electric field, magnetic field, and surface current for the TM mode and TE mode, respectively.</p>
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<p>Different polarization angles and oblique incidence absorption curves for TE and TM modes: (<b>a</b>) TE mode with varying polarization angles. (<b>b</b>) TE mode with oblique incidence of electromagnetic waves. (<b>c</b>) TM mode with varying polarization angles. (<b>d</b>) TM mode with oblique incidence of electromagnetic waves.</p>
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<p>(<b>a</b>) Physical structure (<b>b</b>) Testing environment.</p>
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<p>Experimental and simulation results of 18–26 GHz frequency range. (<b>a</b>) Normal incidence of electromagnetic waves; blue dashed line represents experimental results, and red solid line represents simulation results. (<b>b</b>) Experimental and simulation results for different polarization angles; dash–dot line represents simulation results, and solid line represents experimental results. (<b>c</b>) Experimental and simulation results for oblique incidence; dash–dot line represents simulation results, and solid line represents experimental results.</p>
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11 pages, 9510 KiB  
Article
Compact and Wide-Stopband Bandpass Filter Using Hybrid Shielded EMCSIW and CSRR Resonators with a Mixed Electromagnetic Coupling Scheme
by Zhuo-Wei Miao
Micromachines 2024, 15(12), 1426; https://doi.org/10.3390/mi15121426 - 27 Nov 2024
Viewed by 526
Abstract
This paper presents a bandpass filter (BPF) exploiting hybrid shielded eighth-mode circular substrate-integrated waveguide (SD-EMCSIW) and complementary split ring resonator (CSRR) resonators. The proposed BPF leverages the SD-EMCSIW resonator with a 45-degree angle to create a second-order BPF with a mixed electromagnetic coupling [...] Read more.
This paper presents a bandpass filter (BPF) exploiting hybrid shielded eighth-mode circular substrate-integrated waveguide (SD-EMCSIW) and complementary split ring resonator (CSRR) resonators. The proposed BPF leverages the SD-EMCSIW resonator with a 45-degree angle to create a second-order BPF with a mixed electromagnetic coupling scheme. Detailed analyses of the related electromagnetic characteristics and operating mechanisms have been performed. In order to further reduce the occupied area, the CSRR structures are embedded into the SD-EMCSIW resonators. Meanwhile, extra metallic via-holes are implemented to enhance the upper-stopband performance. A transmission zero (TZ) of the second-order BPF can be placed on either the left or right side of the passband and can be flexibly adjusted. To validate the design concept, a second-order hybrid SD-EMCSIW and CSRR BPF was designed, simulated, fabricated, and measured as a specific example. The prototype operates at a center frequency f0 of 8.3 GHz with a 3 dB fractional bandwidth of 8.1%. Two transmission zeros are located near the right passband. The upper-stopband rejection reaches up to 15 dB at 2.85 times the center frequency f0. Both the simulated and measured results show satisfactory agreement. Meanwhile, the overall size of the proposed hybrid SD-EMCSIW and CSRR BPF is 13.5 mm × 13.0 mm (0.37λ0 × 0.36λ0), featuring a compact physical dimension in the filter design. Full article
(This article belongs to the Special Issue Microwave Passive Components, 2nd Edition)
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<p>Configuration and electric-field distributions of full-mode and sub-mode CSIW resonators. (<b>a</b>) FMCSIW (<b>b</b>) HMCSIW (<b>c</b>) QMCSIW (<b>d</b>) EMCSIW.</p>
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<p>Electric-field distributions of the first three sub-mode CSIW modes: (<b>a</b>) TM<sub>010</sub>, (<b>b</b>) TM<sub>020</sub>, (<b>c</b>) TM<sub>110</sub>.</p>
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<p>Configurations and electric-field distributions of the shielded SD-SMCSIW resonators: (<b>a</b>) SD-HMCSIW, (<b>b</b>) SD-QMCSIW, (<b>c</b>) SD-EMCSIW.</p>
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<p>Electric-field distributions of the first three modes in SD-EMCSIW resonator: (<b>a</b>) TM<sub>010</sub>, (<b>b</b>) TM<sub>020</sub>, (<b>c</b>) TM<sub>110</sub>.</p>
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<p>Configuration of the hybrid SD-EMCSIW and CSRR resonator.</p>
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<p>Configuration and coupling scheme of the second-order SD-EMCSIW BPF with EM coupling. (<b>a</b>) Structure of the second-order SD-EMCSIW BPF with mixed coupling. (<b>b</b>) Coupling scheme.</p>
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<p>Configuration and coupling scheme of the second-order SD-EMCSIW BPF with EM coupling. (<b>a</b>) Structure of the second-order SD-EMCSIW BPF with mixed coupling. (<b>b</b>) Coupling scheme.</p>
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<p>Simulated frequency responses of the second-order SD-EMCSIW BPF versus the location of offset microstrip line <span class="html-italic">L<sub>o</sub></span>.</p>
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<p>Configuration of the second-order hybrid SD-EMCSIW and CSRR BPF in Type II.</p>
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<p>Frequency responses of the second-order hybrid SD-EMCSIW and CSRR BPF in Type II.</p>
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<p>Configuration of the second-order hybrid SD-EMCSIW and CSRR BPF with extra perturbed via-holes in Type III.</p>
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<p>Frequency response of the second-order hybrid SD-EMCSIW and CSRR BPF with extra perturbed via-holes in Type III.</p>
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<p>Photograph of the second-order hybrid SD-EMCSIW and CSRR BPF with mixed EM coupling scheme.</p>
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<p>Simulated and measured frequency responses of the second-order hybrid SD-EMCSIW and CSRR BPF with mixed EM coupling scheme.</p>
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7 pages, 557 KiB  
Proceeding Paper
Generation of Entangled Photon Pairs from High-Quality-Factor Silicon Microring Resonator at Near-Zero Anomalous Dispersion
by Muneeb Farooq, Francisco Soares and Francisco Diaz
Phys. Sci. Forum 2024, 10(1), 2; https://doi.org/10.3390/psf2024010002 - 21 Nov 2024
Viewed by 161
Abstract
The intrinsic third-order nonlinearity in silicon has proven it to be quite useful in the field of quantum optics. Silicon is suitable for producing time-correlated photon pairs that are sources of heralded single-photon states for quantum integrated circuits. A quantum signal source in [...] Read more.
The intrinsic third-order nonlinearity in silicon has proven it to be quite useful in the field of quantum optics. Silicon is suitable for producing time-correlated photon pairs that are sources of heralded single-photon states for quantum integrated circuits. A quantum signal source in the form of single photons is an inherent requirement for the principles of quantum key distribution technology for secure communications. Here, we present numerical simulations of a silicon ring with a 6 μ m radius side-coupled with a bus waveguide as the source for the generation of single photons. The photon pairs are generated by exploring the process of degenerate spontaneous four-wave mixing (SFWM). The free spectral range (FSR) of the ring is quite large, simplifying the extraction of the signal/idler pairs. The phase-matching condition is considered by studying relevant parameters like the dispersion and nonlinearity. We optimize the ring for a high quality factor by varying the gap between the bus and the ring waveguide. This is the smallest ring studied for photon pair generation with a quality factor in the order of 10 5 . The width of the waveguides is chosen such that the phase-matching condition is satisfied, allowing for the propagation of fundamental modes only. The bus waveguide is pumped at one of the ring resonances with the minimum dispersion (1543.5 nm in our case) to satisfy the principle of energy conservation. The photon pair generation rate achieved is comparable to the state of the art. The photon pair sources exploiting nonlinear frequency conversion/generation processes is a promising alternative to atom-like single-photon emitters in the field of integrated photonics. Such miniaturized structures will benefit future on-chip architectures where multiple single-photon source devices are required on the same chip. Full article
(This article belongs to the Proceedings of The 1st International Online Conference on Photonics)
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<p>Mode characteristics: (<b>a</b>) Silicon ring and bus percolated inside silicon dioxide cladding (cross-section). <math display="inline"><semantics> <mrow> <mi>H</mi> <mo>=</mo> <mn>0.5</mn> <mspace width="3.33333pt"/> <mi mathvariant="sans-serif">μ</mi> </mrow> </semantics></math>m. (<b>b</b>) Optical mode profile (magnitude) for a transverse electric (TE) mode in a typical single-mode bent SOI waveguide. The waveguide cross-section is <math display="inline"><semantics> <mrow> <mi>h</mi> <mo>=</mo> <mn>220</mn> </mrow> </semantics></math> nm thick and <math display="inline"><semantics> <mrow> <mi>w</mi> <mo>=</mo> <mn>405</mn> </mrow> </semantics></math> nm wide, with a bent radius <math display="inline"><semantics> <mrow> <mi>r</mi> <mo>=</mo> <mn>6</mn> <mspace width="3.33333pt"/> <mi mathvariant="sans-serif">μ</mi> </mrow> </semantics></math>m.</p>
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<p>Ring characteristics: (<b>a</b>) Variation in dispersion for ring cross-section with different waveguide widths. (<b>b</b>) Transmission spectrum at <math display="inline"><semantics> <mrow> <mi>w</mi> <mo>=</mo> <mn>405</mn> </mrow> </semantics></math> nm and gap of 270 nm.</p>
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<p>Nonlinear response: (<b>a</b>) Normalized power spectrum from the varFDTD analysis showing the emergence of idler/converted. (<b>b</b>) Variation in <math display="inline"><semantics> <mi mathvariant="script">R</mi> </semantics></math> with pump power (logarithmic scale).</p>
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