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15 pages, 5061 KiB  
Article
Spatially Variable Ripple and Groove Formation on Gallium Arsenide Using Linear, Radial, and Azimuthal Polarizations of Laser Beam
by Kalvis Kalnins, Vyacheslav V. Kim, Andra Naresh Kumar Reddy, Anatolijs Sarakovskis and Rashid A. Ganeev
Photonics 2024, 11(8), 710; https://doi.org/10.3390/photonics11080710 - 30 Jul 2024
Viewed by 308
Abstract
We demonstrated the linear, radial, and annular ripple formation on the surface of GaAs. The formation of linear ripples was optimized by the number of shots and the fluence of 30 ps, 532 nm pulses. The radial and annular nanoripples were produced under [...] Read more.
We demonstrated the linear, radial, and annular ripple formation on the surface of GaAs. The formation of linear ripples was optimized by the number of shots and the fluence of 30 ps, 532 nm pulses. The radial and annular nanoripples were produced under the ablation using doughnut-like beams possessing azimuthal and radial polarizations, respectively. We compare the ripples and grooves formed by a linearly polarized Gaussian beam relative to an annular vector beam. The joint overlap of sub-wavelength grooves with ripples formed by azimuthally and radially polarized beams was reported. The conditions under which the shape of radial and ring-like nano- or micro-relief on the GaAs surface can be modified by modulating the polarization of laser pulse were determined. The resultant surface processing of GaAs using a laser beam with different polarization modes is useful for exploring valuable insights and benefits in different applications. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Experimental scheme for LIPSS formation on the surface of GaAs using 532 nm, 30 ps pulses. The bottom insets show the spatial shapes of (<b>b</b>) a linearly polarized Gaussian beam, (<b>c</b>) a radially polarized annular beam, and (<b>d</b>) an azimuthally polarized annular beam and (<b>e</b>–<b>g</b>) their corresponding line-outs of spatial distribution. White arrows are the directions of polarization.</p>
Full article ">Figure 2
<p>SEM images of ablated GaAs using (<b>a</b>) 5 shots, (<b>b</b>) 15 shots, and (<b>c</b>) 25 shots of 532 nm, 30 ps pulses at the fluence 0.18 J cm<sup>−2</sup> on the target surface. The bottom panels of (<b>a</b>–<b>c</b>) correspond to the enlarged parts of the corresponding areas marked in red. White lines correspond to 10 μm. Blue arrows show the direction of polarization of the Gaussian beam.</p>
Full article ">Figure 3
<p>(<b>a</b>) Appearance of orthogonally directed lines (HSFL) with a smaller spatial period at a larger number of shots (30) on the same place of GaAs. (<b>b</b>) Enlarged part of <a href="#photonics-11-00710-f003" class="html-fig">Figure 3</a>a. The blue arrow shows the direction of polarization of the laser beam. The white line corresponds to 1 μm. The average spatial periods of orthogonal (LSFL and HSFL) ripples were 480 and 270 nm, respectively.</p>
Full article ">Figure 4
<p>(<b>a</b>) Spatial shape of the ablated area on the surface of GaAs by the doughnut-like beam with a radial distribution of polarization (white arrows). (<b>b</b>) The enlarged square of <a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>a shows the part of the ablated ring dominated by the presence of the grooves growing parallel to the polarization. (<b>c</b>) An enlarged part of <a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>b shows the inner region of the ring. One can see the rings of ripples, followed by the grooves. These ripples remain almost unchanged on the right side of <a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>c while appearing under the grooves. (<b>d</b>) The enlarged part of <a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>b shows the outer region of the ring. One can see the LSFL at the smallest fluence of the laser beam, followed by the appearance of the grooves above the rings on the left side of <a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>d. The white bars correspond to 40 μm (<a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>a) and 10 μm (<a href="#photonics-11-00710-f004" class="html-fig">Figure 4</a>b–d).</p>
Full article ">Figure 5
<p>(<b>a</b>) The shape of the ablated area using the radially polarized beam at F = 0.18 J cm<sup>−2</sup> and N = 5. (<b>b</b>) Enlarged part of <a href="#photonics-11-00710-f005" class="html-fig">Figure 5</a>a showing the ring-like LSFL throughout the ablation area. The white bars correspond to 60 μm (<a href="#photonics-11-00710-f005" class="html-fig">Figure 5</a>a) and 10 μm (<a href="#photonics-11-00710-f005" class="html-fig">Figure 5</a>b). While arrows show the direction of polarization of the laser beam.</p>
Full article ">Figure 6
<p>(<b>a</b>) SEM image of the whole area of ablation using 20 shots of the azimuthally polarized beam. Almost the whole ablated area was filled in with grooves. (<b>b</b>,<b>c</b>) Enlarged parts of the ablated area and outer border of the ablated area, respectively. The ripples were observed only in the area of the outer border of the ablation. (<b>d</b>) SEM image of the whole area of ablation using 5 shots of the azimuthally polarized beam at the same fluence of heating radiation (F = 0.22 J cm<sup>−2</sup>) as in the case shown in <a href="#photonics-11-00710-f006" class="html-fig">Figure 6</a>a. (<b>e</b>,<b>f</b>) Enlarged parts of the ablated area and inner border of the ablated area, respectively. LSFL, in that case, dominated along the whole ablated area. The white bars correspond to 80 μm (<a href="#photonics-11-00710-f006" class="html-fig">Figure 6</a>a,d) and 10 μm (<a href="#photonics-11-00710-f006" class="html-fig">Figure 6</a>c,f). While arrows show the direction of polarization of the laser beam.</p>
Full article ">Figure 7
<p>(<b>a</b>,<b>d</b>) The intensity profiles of the linearly polarized Gaussian beam and radially polarized beam, respectively. (<b>b</b>,<b>e</b>) The corresponding images of ablated areas. (<b>c</b>,<b>f</b>) The enlarged parts of the red squares are marked in <a href="#photonics-11-00710-f007" class="html-fig">Figure 7</a>b and <a href="#photonics-11-00710-f007" class="html-fig">Figure 7</a>e, respectively. Blue arrows show the direction of polarization of the laser beam.</p>
Full article ">Figure 8
<p>Left panels of <a href="#photonics-11-00710-f008" class="html-fig">Figure 8</a>a,b: the images of the ablation areas after laser–matter interaction in the case of the rotation of the S-waveplate by (<b>a</b>) 22.5° and (<b>b</b>) 45° from the position corresponding to the pure radial polarization of the annular beam. The enlarged images of the ablation areas in these two cases are shown in the right panels. Red curved lines show the leaned directions of polarizations at different points of the ablation. The grooves follow these leaned directions of polarization.</p>
Full article ">
20 pages, 15998 KiB  
Article
AscentAM: A Software Tool for the Thermo-Mechanical Process Simulation of Form Deviations and Residual Stresses in Powder Bed Fusion of Metals Using a Laser Beam
by Dominik Goetz, Hannes Panzer, Daniel Wolf, Fabian Bayerlein, Josef Spachtholz and Michael F. Zaeh
Modelling 2024, 5(3), 841-860; https://doi.org/10.3390/modelling5030044 - 15 Jul 2024
Viewed by 599
Abstract
Due to the tool-less fabrication of parts and the high degree of geometric design freedom, additive manufacturing is experiencing increasing relevance for various industrial applications. In particular, the powder bed fusion of metals using a laser beam (PBF-LB/M) process allows for the metal-based [...] Read more.
Due to the tool-less fabrication of parts and the high degree of geometric design freedom, additive manufacturing is experiencing increasing relevance for various industrial applications. In particular, the powder bed fusion of metals using a laser beam (PBF-LB/M) process allows for the metal-based manufacturing of complex parts with high mechanical properties. However, residual stresses form during PBF-LB/M due to high thermal gradients and a non-uniform cooling. These lead to a distortion of the parts, which reduces the dimensional accuracy and increases the amount of post-processing necessary to meet the defined requirements. To predict the resulting residual stress state and distortion prior to the actual PBF-LB/M process, this paper presents the finite-element-based simulation tool AscentAM with its core module and several sub-modules. The tool is based on open-source programs and utilizes a sequentially coupled thermo-mechanical simulation, in which the significant influences of the manufacturing process are considered by their physical relations. The simulation entirely emulates the PBF-LB/M process chain including the heat treatment. In addition, algorithms for the part pre-deformation and the export of a machine-specific file format were implemented. The simulation results were verified, and an experimental validation was performed for two benchmark geometries with regard to their distortion. The application of the optimization sub-module significantly minimized the form deviation from the nominal geometry. A high level of accuracy was observed for the prediction of the distortion at different manufacturing states. The process simulation provides an important contribution to the first-time-right manufacturing of parts fabricated by the PBF-LB/M process. Full article
(This article belongs to the Special Issue Finite Element Simulation and Analysis)
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Figure 1

Figure 1
<p>Schematic representation of the workflow of the simulation tool <span class="html-italic">AscentAM</span> shown for the core module with the implemented functional blocks and the optional sub-modules.</p>
Full article ">Figure 2
<p>Schematic representation of (<b>a</b>) an FE mesh, whose elements are sorted into several LCs by their center of gravity, and (<b>b</b>) the applied flash exposure heat source at a currently active LC showing the melting temperature <math display="inline"><semantics> <msub> <mi>T</mi> <mi mathvariant="normal">M</mi> </msub> </semantics></math>, the process temperature <math display="inline"><semantics> <msub> <mi>T</mi> <mi mathvariant="normal">P</mi> </msub> </semantics></math>, the build platform temperature <math display="inline"><semantics> <msub> <mi>T</mi> <mi>BP</mi> </msub> </semantics></math> and the corresponding thermal gradient during the heating step; <span class="html-italic">z</span>: build direction.</p>
Full article ">Figure 3
<p>Modeling approach for the separation of the part from the build platform, exemplarily represented by twelve sequential computational steps, for each of which the interface elements are deactivated; <span class="html-italic">z</span>: build direction.</p>
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<p>True-to-scale representation of (<b>a</b>) the academic cantilever beam and (<b>b</b>) the topology-optimized bracket geometry with the marked verification points (VPs), each used for the mesh convergence study; dimensions in mm; <span class="html-italic">z</span>: build direction.</p>
Full article ">Figure 5
<p>True-to-scale top view of the build platforms indicating the positions of (<b>a</b>) the cantilever beams and (<b>b</b>) the brackets; exemplary representation of the local coordinate systems for each of the parts placed on the respective build platform (250 × 250 mm<sup>2</sup>).</p>
Full article ">Figure 6
<p>Simulation results of the cantilever beam depicted without the build platform for an FE size <math display="inline"><semantics> <mrow> <mi>e</mi> <mo>=</mo> <mn>0.50</mn> </mrow> </semantics></math> mm and an LC height <math display="inline"><semantics> <mrow> <mi>L</mi> <mo>=</mo> <mn>1.00</mn> </mrow> </semantics></math> mm; representation of the thermal results for (<b>a</b>) the heating step, (<b>c</b>) the first cooling step, (<b>e</b>) the fourth cooling step and (<b>g</b>) the tenth cooling step of the last LC; mechanical results shown with a five-fold scaling for (<b>b</b>) the heating step, (<b>d</b>) the first cooling step, (<b>f</b>) the fourth cooling step and (<b>h</b>) the tenth cooling step of the last LC; <span class="html-italic">z</span>: build direction.</p>
Full article ">Figure 7
<p>Mesh convergence results for the cantilever beam showing a converging behavior with decreasing the LC height and the FE size; nomenclature at selected evaluation points: (LC height <span class="html-italic">L</span>|FE size <span class="html-italic">e</span>).</p>
Full article ">Figure 8
<p>Measured form deviation between the nominal and the as-built cantilever beam after the separation (<b>a</b>) without applying the simulative pre-deformation algorithm and (<b>b</b>) using the simulative pre-deformation algorithm from the optimization sub-module; missing data points indicated by gray color; <span class="html-italic">z</span>: build direction.</p>
Full article ">Figure 9
<p>Form deviation of the bracket geometry (<b>a</b>) between the nominal geometry and the as-built part before SRA, (<b>b</b>) between the nominal geometry and the simulation result before SRA, (<b>c</b>) between the nominal geometry and the as-built part after SRA and (<b>d</b>) between the nominal geometry and the simulation result after SRA; missing data points indicated by gray color; <span class="html-italic">z</span>: build direction.</p>
Full article ">
12 pages, 2808 KiB  
Article
High–Speed Laser Modulation for Low–Noise Micro–Cantilever Array Deflection Measurement
by Weiwei Xue, Yong Su and Qingchuan Zhang
Photonics 2024, 11(7), 619; https://doi.org/10.3390/photonics11070619 - 28 Jun 2024
Viewed by 335
Abstract
In this paper, an innovative approach is introduced to address the noise issues associated with micro–cantilever array deflection measurement systems employing multiple lasers. Conventional systems are affected by laser mode hopping during switching, resulting in wavelength instability and beam spot fluctuations that take [...] Read more.
In this paper, an innovative approach is introduced to address the noise issues associated with micro–cantilever array deflection measurement systems employing multiple lasers. Conventional systems are affected by laser mode hopping during switching, resulting in wavelength instability and beam spot fluctuations that take several hundred milliseconds to stabilize. To mitigate these limitations, a high–speed laser modulation technique is utilized, leveraging the averaging effect over multiple modulation cycles within the sampling window. By driving the lasers with a high–frequency carrier signal, a low–noise and stable output suitable for micro–cantilever beam deflection measurement is achieved. The effectiveness of this approach is demonstrated by simultaneously modulating the lasers and rapidly observing the spectral and centroid variations during high–speed switching using a custom–built high–speed spectrometer. The centroid fluctuations are also analyzed under different modulation frequencies. The experimental results confirm that the high–speed modulation method can reduce the standard deviation of beam spot fluctuations by more than 90%, leading to significant improvements in noise reduction compared to traditional laser switching methods. The proposed high–speed laser modulation approach offers a promising solution for enhancing the precision and stability of multi–laser micro–cantilever array deflection measurement systems. Full article
(This article belongs to the Special Issue Recent Advances in 3D Optical Measurement)
Show Figures

Figure 1

Figure 1
<p>An illustration of the laser spot centroid position variation in a microcantilever beam system. The left diagram shows a schematic of the microcantilever array and laser optical path, with the microcantilever array drawn to scale. The right side shows the centroid position variation curve over time after laser activation, along with snapshots of the laser spot at different moments.</p>
Full article ">Figure 2
<p>(<b>a</b>) A schematic of the microcantilever system. (<b>b</b>) A 3D model of the cell body and a photograph of the microcantilever array with a 1 mm scale bar. (<b>c</b>) A laser switching strategy and timing diagram. (<b>d</b>) A schematic of lasers sequentially illuminating different tips of the microcantilever array.</p>
Full article ">Figure 3
<p>The electrical connections, circuit design, and optical detection setup. (<b>a</b>) A schematic of the electrical connection. (<b>b</b>) A photograph of the circuit boards, multiple lasers, and V–groove array. (<b>c</b>) A schematic of the custom–built 100 kHz spectrometer. (<b>d</b>) A photograph of the custom–built spectrometer.</p>
Full article ">Figure 4
<p>The laser spectra and centroid spot position measurements with and without modulation. (<b>a</b>) An unmodulated laser spectrum over 2 s, captured at 100 Hz with a 10 ms exposure time. (<b>b</b>) A 1 kHz square wave modulated laser spectrum over 2 s, captured at 100 Hz. (<b>c</b>) A 1 kHz modulated laser spectrum observed at 100 kHz with a 10 μs exposure time, showing periodic behavior within the individual modulation periods. The laser is operated with an 80% duty cycle. (<b>d</b>) The unmodulated laser centroid position variation, captured with a 10 ms sampling window for improved accuracy and noise reduction. (<b>e</b>) A 1 kHz modulated laser centroid position variation, captured with a 10 ms sampling window, integrating multiple modulation periods. (<b>f</b>) A 1 kHz modulated laser centroid position observed at 100 kHz, revealing the high–speed dynamics within each on/–off cycle.</p>
Full article ">Figure 5
<p>(<b>a</b>) Comparison of spot position curves under 1 kHz and 100 kHz sinusoidal modulation. (<b>b</b>) Standard deviation of spot position fluctuations over time for different frequencies and waveforms, including direct switching without any modulation (Direct SW), sinusoidal modulation (Sin), and square wave modulation (SQR). (<b>c</b>) Average standard deviation of the first 30 elements (0–300 ms) for different modulation conditions.</p>
Full article ">Figure 6
<p>(<b>a</b>) Unmodulated temperature response: The temperature gradient ranges from 25.0 °C to 25.2 °C, with substantial noise present due to the laser switching instability. The sampling rate is 0.4 Hz. (<b>b</b>) Modulated temperature response with 100 kHz high–frequency laser modulation: A significant reduction in noise is observed, resulting in a smoother and more stable response. The sampling rate is increased to 6.25 Hz.</p>
Full article ">
12 pages, 2659 KiB  
Article
Refraction-Based Laser Scanning Microcantilever Array System
by Weiwei Xue, Yong Su and Qingchuan Zhang
Photonics 2024, 11(7), 592; https://doi.org/10.3390/photonics11070592 - 25 Jun 2024
Viewed by 673
Abstract
Microcantilever arrays are valuable tools for detecting minute physical and chemical changes. Traditional microcantilever array systems, including our previous work utilizing multiple laser arrays, frequently encounter high complexity, significant costs, and increased noise caused by laser switching. This study introduces a refraction-based laser [...] Read more.
Microcantilever arrays are valuable tools for detecting minute physical and chemical changes. Traditional microcantilever array systems, including our previous work utilizing multiple laser arrays, frequently encounter high complexity, significant costs, and increased noise caused by laser switching. This study introduces a refraction-based laser scanning system that significantly mitigates these issues by employing a rotating glass optical block for multiplex scanning. This innovative approach not only simplifies the scanning process by eliminating the need to move the laser source or the microcantilever array but also enhances scanning speed and reduces noise, as demonstrated by our experiments. Overall, this research implements a new optical scanning strategy for microcantilever array systems, which is promising due to its direct application potential as it paves the way for more accurate, high-performing, and cost-effective sensing solutions. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Principle of refraction-based deflection. (<b>b</b>) Relationship between the incident angle <span class="html-italic">θ</span>₁ and beam shift d for a glass with a thickness of 10 mm and a refractive index of 1.515. (<b>c</b>) Schematic diagram of the experimental setup. The laser light is deflected towards different tips of the microcantilevers by rotating the refractive optical block.</p>
Full article ">Figure 2
<p>(<b>a</b>) Schematic diagram of the system. (<b>b</b>) A photograph of the experimental setup. (<b>c</b>) A 3D model of the microcantilever beam chamber is shown, with an inset photograph of the microcantilever sensor with a 1 mm scale bar.</p>
Full article ">Figure 3
<p>(<b>a</b>) Displacement curves post-switch of the refraction scanning (blue) and laser switching devices (red). (<b>b</b>) The standard deviation of the displacement. (<b>c</b>) Timing Diagram of Control Operations.</p>
Full article ">Figure 4
<p>(<b>a</b>) Plot of the light spot centroid position on the detector over 10 s with and without the deflector. Similar displacement magnitudes indicate the minimal impact of the stepped deflector on the centroid position. (<b>b</b>) Demonstration of the system’s dynamic positioning repeatability during the deflector switching cycle (10 s:9 s at the desired position, 1 s away). Minimal disturbance to centroid detection and highly consistent overall trend maintained, despite raw curve discontinuities. (<b>c</b>) Displacement of the cantilever beam tip over time when comparing the noise levels between the refraction scanning readout device and a laser switching readout device at rest. (<b>d</b>) Noise spectrum of the two devices across different frequencies.</p>
Full article ">Figure 5
<p>Performance of proposed system in physical and chemical sensing. (<b>a</b>) Displacement of microcantilevers caused by thermal stages, captured by the refraction scanning (blue lines) and laser switching readout (red lines) devices. (<b>b</b>) The deflection responses of the microcantilever to carcinoembryonic antigen (CEA) concentrations of 0 ng/mL (control), 100 ng/mL, and 200 ng/mL. Lighter colors represent the deflection of individual microcantilevers, while darker colors indicate the average deflection.</p>
Full article ">
12 pages, 4617 KiB  
Article
Generating Optical Vortex Array Laser Beams of Superimposing Hermite–Gaussian Beams with a Dual–Phase Modulation Digital Laser System
by Ly Ly Nguyen Thi, Ko-Fan Tsai and Shu-Chun Chu
Photonics 2024, 11(6), 563; https://doi.org/10.3390/photonics11060563 - 15 Jun 2024
Viewed by 662
Abstract
This study presents an efficient and practical intra-cavity approach for selectively generating vortex array laser beams employing a dual-phase modulation digital laser system, which has not yet been completed in single-phase modulation digital laser. The stable optical vortex array laser beams were formed [...] Read more.
This study presents an efficient and practical intra-cavity approach for selectively generating vortex array laser beams employing a dual-phase modulation digital laser system, which has not yet been completed in single-phase modulation digital laser. The stable optical vortex array laser beams were formed by superimposing cavity Hermite–Gaussian (HG) eigenmodes. In particular, when the selected cavity HG modes shared the same Gouy phase, the resulting optical vortex beam could preserve its light field pattern, thereby maintaining the optical vortex properties in the near and far fields. Numerical results demonstrated that employing dual-phase modulation could establish optimal boundary conditions for the selection of HG modes within the cavity, successfully generating various vortex array laser beams. The experimental validation of the proposed method confirmed the ability to select optical vortex array lasers solely by controlling the loaded phase of the dual-phase modulation digital laser. These results demonstrate the ability of digital lasers to generate and dynamically control optical vortex array lasers. Full article
(This article belongs to the Special Issue Optical Vortex Laser)
Show Figures

Figure 1

Figure 1
<p>Some vortex arrays formed by different combinations of the degenerated family of Hermite–Gaussian (HG) modes. Theoretical results for the (<b>a</b>) amplitude and (<b>b</b>) phase of the vortex array at beam waist positions are presented.</p>
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<p>(<b>a</b>) The laser light measurement and the digital laser setup with an example SLM loaded phase diagram for generating vortex array formed by <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> </mrow> </semantics></math>. The red dotted box shows the dual-SLM digital cavity. (<b>b</b>) A schematic diagram of an equivalent SLM-SLM laser resonator simplified from the experiment laser resonator.</p>
Full article ">Figure 3
<p>Simulation results of the <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math> mode generation via SLM-SLM cavity. (<b>a</b>) The phase diagram on the SLM for generating the <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math> mode. (<b>b</b>) The amplitude of a convergent optical vortex array comprising the <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math> mode. (<b>c</b>) The phase development of the intra-cavity light field from a random phase beam to the <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>11</mn> </mrow> </msub> <mo> </mo> </mrow> </semantics></math> mode while propagating inside the cavity with dual-phase modulation.</p>
Full article ">Figure 4
<p>The experimental results for the vortex array beam formed by superimposing degenerated family Hermite–Gaussian (HG) modes shown in <a href="#photonics-11-00563-f001" class="html-fig">Figure 1</a>. (<b>a</b>,<b>b</b>) are the intensity profile and their corresponding interference pattern with plane wave, respectively. (<b>c</b>) are the numerical results of the interference pattern of the five ideal vortex arrays with plane waves.</p>
Full article ">Figure 5
<p>The experimental results for the far-field beam profile of the vortex array of the five degenerated families of the Hermite–Gaussian (HG) modes. The intensity profile (<b>a</b>) and their corresponding interference pattern (<b>b</b>) with plane wave, respectively.</p>
Full article ">Figure 6
<p>The beam profile at the far field and near field of vortex array from a different family of Hermite–Gaussian (HG) modes, <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>30</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>22</mn> </mrow> </msub> </mrow> </semantics></math>. The numerical (<b>a</b>) and experimental (<b>b</b>) results, respectively.</p>
Full article ">Figure 7
<p>More results on the superposition of the Hermite–Gaussian (HG) modes from different families. The theoretical results for the near and far field intensity pattern of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>01</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>20</mn> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>02</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>30</mn> </mrow> </msub> </mrow> </semantics></math> (<b>a</b>) and the corresponding experimental results (<b>b</b>).</p>
Full article ">Figure 8
<p>The intensity (<b>a</b>) and interference pattern (<b>b</b>) vortex array formed by the <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>21</mn> </mrow> </msub> <mo>+</mo> <mi>i</mi> <msub> <mrow> <mi>H</mi> <mi>G</mi> </mrow> <mrow> <mn>12</mn> </mrow> </msub> </mrow> </semantics></math> modes at different pump powers.</p>
Full article ">
9 pages, 3269 KiB  
Technical Note
Design and Test of a Klystron Intra-Pulse Phase Feedback System for Electron Linear Accelerators
by Luca Piersanti, Marco Bellaveglia, Fabio Cardelli, Alessandro Gallo, Riccardo Magnanimi, Sergio Quaglia, Michele Scampati, Giorgio Scarselletta, Beatrice Serenellini and Simone Tocci
Photonics 2024, 11(5), 413; https://doi.org/10.3390/photonics11050413 - 29 Apr 2024
Viewed by 674
Abstract
Beam stability and timing jitter in modern linear accelerators are becoming increasingly important. In particular, if a magnetic or radio-frequency (RF) compression regime is employed, the beam time of arrival jitter at the end of the linac can be strictly correlated with the [...] Read more.
Beam stability and timing jitter in modern linear accelerators are becoming increasingly important. In particular, if a magnetic or radio-frequency (RF) compression regime is employed, the beam time of arrival jitter at the end of the linac can be strictly correlated with the phase noise of the accelerating fields of the RF structure working off-crest. For this reason, since 2008, an RF fast-feedback technique, which acts within each RF pulse, has been successfully employed at LNF-INFN (Laboratori Nazionali di Frascati dell’Istituto Nazionale di Fisica Nucleare) in the SPARC_LAB (Sources for Plasma Accelerators and Radiation Compton with Laser And Beam) facility on S-band (2856 MHz) klystrons powered by pulse-forming network (PFN) modulators, as reported in this paper. However, in order to meet the more stringent requirements of plasma wakefield acceleration schemes, some upgrades to this feedback system have been recently carried out. The first prototype has been experimentally tested on a C-band (5712 MHz) klystron, driven by a solid-state modulator, in order to investigate the possibility for additional improvement resulting from the inherently more stable power source. In this paper, the design, realization and the preliminary measurement results obtained at SPARC_LAB after such upgrades will be reviewed. Full article
(This article belongs to the Special Issue Recent Advances in Free Electron Laser Accelerators)
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<p>The state of the art for measured phase stability in pulsed RF plants worldwide is compared with the facilities at LNF-INFN. The solid fill color represents the best results published or disseminated by other laboratories, while the transparent fill color accounts for the spread between the worst- and best-case scenarios when multiple plants are available.</p>
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<p>SPARC_LAB klystron n.2 (K2) RF system. Highlighted block diagram of the fast intra-pulse feedback that includes the solid state driver amplifier (D2) and the Binary Phase Shift Keying (BPSK), which realizes the phase jump for the pulse compressor that feeds the two accelerating sections (S1 and S2). Moreover, a screenshot of its control system with the typical phase detector and error amplifier output signals is reported at the bottom.</p>
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<p>Recent measurement at SPARC_LAB of the S-band fast intra-pulse feedback capability with Libera LLRF front-end. The klystron phase measured with feedback off is shown in blue, whereas that with feedback on is shown in orange. There are approximatively 200 shots at 10 Hz repetition rate. A jitter reduction down to <math display="inline"><semantics> <mrow> <mn>0.046</mn> </mrow> </semantics></math> deg <span class="html-small-caps">rms</span> has been obtained, with an overall compression of a factor &gt; 4.</p>
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<p>New error amplifier board (<b>left</b>) and the new RF chassis (<b>right</b>) realized at INFN-LNF laboratories for the klystron loop upgrade.</p>
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<p>(<b>a</b>) Block diagram of the laboratory experimental setup for the klystron loop bench test, and (<b>b</b>) oscilloscope capture of the functionality of the slow feedback. The error amplifier output without slow feedback is shown in orange; the same output with slow feedback in operation is shown in blue. It can be clearly seen that the loop also allows us to reach a phase value close to the desired one when the RF pulse is off. This minimizes the transient and the overall phase modulation required to reach the steady state, as shown in the waveform zoom.</p>
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<p>Intra-pulse feedback prototype measurement results at SPARC_LAB facility on the C-band power plant. In bold the results obtained with the new feedback on.</p>
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17 pages, 6834 KiB  
Article
A Novel Inserting Pilot Radio over Fiber System without the Bit Walk-Off Effect for the Generation and Distribution of Frequency 16-Tupling Millimeter Waves by Mach–Zehnder Modulators
by Xu Chen, Xinqiao Chen, Siyuan Dai, Bin Li and Ling Wang
Photonics 2024, 11(5), 410; https://doi.org/10.3390/photonics11050410 - 28 Apr 2024
Viewed by 879
Abstract
A novel inserting pilot scheme to generate and distribute a frequency 16-tupling millimeter wave (MMW) radio over fiber (ROF) system without the bit walk-off effect via Mach–Zehnder modulators (MZMs) is proposed. The operation principle is analyzed and the feasibility of our proposed scheme [...] Read more.
A novel inserting pilot scheme to generate and distribute a frequency 16-tupling millimeter wave (MMW) radio over fiber (ROF) system without the bit walk-off effect via Mach–Zehnder modulators (MZMs) is proposed. The operation principle is analyzed and the feasibility of our proposed scheme is verified by simulation test. The main part of our scheme is a ±8th-order sidebands generator (SG), which is constructed by four MZMs connected in parallel. In the back-to-back (BTB) transmission case, by properly adjusting the voltage and initial phase of the radio frequency (RF) drive signals of the MZMs, ±8th-order sidebands are generated by the SG. In the data transmission case, the data signal is first split into two beams, one of which modulates the RF drive signal with an electrical phase modulator (PM) while the other is amplified by an electrical gainer (EG), and then the two beams are combined into one and used as the composite RF drive signal of the MZMs. By adjusting the modulation index of the PM and the gain of the EG, the data signal can only be modulated to the +8th-order sideband of the output of the SG. The optical carrier from the continuous wave (CW) laser is split into two paths: one is sent into the SG, and the other is used as a pilot signal. The output signal of SG is combined with the pilot signal and is transmitted to the base station (BS) via optical fiber. At the BS, the pilot signal is filtered out by a fiber Bragg grating (FBG) and used as the carrier for the uplink for carrier reuse. After filtering out the pilot, the signal from the FBG, which is composed of ±8th-order sidebands, is injected into a photodetector, and a frequency 16-tupling MMW with downlink data is generated. The key parameters’ influence on the bit error rate (BER) and Q factor in the system is also analyzed. Our scheme can not only effectively overcome the bit walk-off effect caused by optical fiber chromatic dispersion and greatly increase the fiber transmission distance but can also effectively improve the performance and the tunability of system. Therefore, it has important application prospects in ROF systems. Full article
(This article belongs to the Section Optical Communication and Network)
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<p>Schematic diagram of the structure of the frequency 16-tupling MMW ROF system.</p>
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<p>Schematic diagram of the composite RF signal module, the ±8<sup>th</sup>-order sideband generator module, and the data recovery module.</p>
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<p>Optical spectrum at the output of the 8<sup>th</sup>-order sideband generator (Point A) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Optical spectrum at the output of the CS (Point B) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Optical spectrum at the output of the FBG (Point C) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Optical spectrum at the output of the OA (Point D) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Spectrum at the output of the PD1 (Point E) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Spectrum at the output of the PD2 (Point F) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>The relationship of the Q factor with the transmission distance of the fiber.</p>
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<p>The relationship between the BER and the received power of PD in the downlink and uplink: (<b>a</b>) downlink; (<b>b</b>) uplink.</p>
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<p>Optical spectrum at the output of the 8<sup>th</sup>-order sideband generator (Point A) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Spectrum at the output of the PD1 (Point E) in <a href="#photonics-11-00410-f001" class="html-fig">Figure 1</a>.</p>
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<p>Eye diagram at difference transmission distances: (<b>a</b>) BTB; (<b>b</b>) 6 km; (<b>c</b>) 12 km; (<b>d</b>) 18.6 km.</p>
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<p>Eye diagrams at different transmission distances in our scheme: (<b>a</b>) BTB; (<b>b</b>) 20 km; (<b>c</b>) 40 km; (<b>d</b>) 60 km.</p>
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<p>The relationship of the BER of the downlink with the received power of PD1.</p>
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<p>Relation between the Q factor and extinction ratio.</p>
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<p>Relation between the Q factor and phase modulation index.</p>
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<p>Relation between the G of EG and system Q factor.</p>
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<p>Relation of the Q factor with the P and the G.</p>
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9 pages, 3493 KiB  
Article
Study on Spectrum Shifting and Pulse Splitting of Mode-Locked Fiber Lasers Based on NPR Technology
by Zhenhua Hao, Yu Hu, Siyu Zhou, Jinhui Liu, Xiaohui Li, Yishan Wang and Cunxiao Gao
Nanomaterials 2024, 14(9), 739; https://doi.org/10.3390/nano14090739 - 23 Apr 2024
Cited by 1 | Viewed by 999
Abstract
We conducted a systematic investigation into the spectral and pulse characteristics of C and L-band Nonlinear Polarization Rotation (NPR) mode-locked fiber lasers effectively employing nonlinear polarization rotation technology. In our experimental setup, we achieved a stable mode-locked state at 1560.076 nm, exhibiting a [...] Read more.
We conducted a systematic investigation into the spectral and pulse characteristics of C and L-band Nonlinear Polarization Rotation (NPR) mode-locked fiber lasers effectively employing nonlinear polarization rotation technology. In our experimental setup, we achieved a stable mode-locked state at 1560.076 nm, exhibiting a 3 dB spectral bandwidth of 9.1 nm. As the pump power increased, we observed spectral shifts accompanied by shifts in the first Kelly sideband and the generation of new Kelly sidebands. In this paper, the phenomenon of spectral deviation is elucidated through the interplay of self-phase modulation, group velocity drift, and polarization-dependent isolator (PD-ISO) filter effect, with an analysis of the formation and deviation of Kelly sidebands. Notably, spectral shift persisted even when the pump power exceeded 200 mW. However, continuous pump power escalation led to soliton splitting, resulting in the formation of new soliton beams. Based on the simultaneous generation of spectral shift and pulse splitting, our study contributes to an enhanced understanding of soliton dynamics in ultrafast fiber lasers and lays a foundation for the application of high-repetition-frequency harmonic mode-locked lasers with tunable wavelengths. Full article
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<p>Schematic diagram of experimental setup. WDM: wavelength division multiplexer; OC: output coupler; EDF: erbium-doped fiber; PC: polarization controller; PD-ISO: polarization-related isolator.</p>
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<p>Pulse characteristics of stable soliton states. (<b>a</b>) Spectra; (<b>b</b>) pulse sequence; (<b>c</b>) spectrum sequence; (<b>d</b>) fundamental frequency signal.</p>
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<p>The spectrum and the pulse characteristics without changing the PC. (<b>a</b>) Increase the pump power to 80 mW, 110 W, and 140 mW for the output light spectrum; (<b>b</b>) enlarged first Kelly sideband K1; (<b>c</b>) single pulse sequence; (<b>d</b>) the relationship between pump power and the position of center wavelength and Kelly sidebands.</p>
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<p>(<b>a</b>) The spectrum when increasing the pump power to 200 mW, 220 W, 230 mW, and 250 mW; (<b>b</b>) enlarged first Kelly sideband.</p>
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<p>Pulse sequences with different numbers of solitons under pump powers ranging from 200 mW to 255 mW.</p>
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13 pages, 7129 KiB  
Article
108 m Underwater Wireless Optical Communication Using a 490 nm Blue VECSEL and an AOM
by Ruiyang Tian, Tao Wang, Xiaoyu Shen, Renjiang Zhu, Lidan Jiang, Yongle Lu, Huanyu Lu, Yanrong Song and Peng Zhang
Sensors 2024, 24(8), 2609; https://doi.org/10.3390/s24082609 - 19 Apr 2024
Cited by 1 | Viewed by 896
Abstract
Advanced light sources in the blue-green band are crucial for underwater wireless optical communication (UWOC) systems. Vertical-external-cavity surface-emitting lasers (VECSELs) can produce high output power and good beam quality, making them suitable for UWOC. This paper presents a 108 m distance UWOC based [...] Read more.
Advanced light sources in the blue-green band are crucial for underwater wireless optical communication (UWOC) systems. Vertical-external-cavity surface-emitting lasers (VECSELs) can produce high output power and good beam quality, making them suitable for UWOC. This paper presents a 108 m distance UWOC based on a 100 mW 490 nm blue VECSEL and an acousto-optic modulator (AOM). The high-quality beam, which is near diffraction-limited, undergoes relatively small optical attenuation when using a conventional avalanche photodiode (APD) as the detector and employing 64-pulse position modulation (PPM). At the time-slot frequency of 50 MHz, the bit error rate (BER) of the UWOC was 2.7 × 10−5. This is the first reported AOM-based UWOC system with a transmission distance over 100 m. The estimated maximum transmission distance may be improved to about 180 m by fully utilizing the detection accuracy of the APD according to the measured attenuation coefficient of the blue VECSEL used. This type of UWOC system, composed of a high-beam-quality light source and a conventional detector, make it more closely suited to practical applications. Full article
(This article belongs to the Section Communications)
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<p>(<b>a</b>) Schematic and (<b>b</b>) photograph of the 490 nm Vertical-external-cavity surface-emitting laser (VECSEL); The LBO in the figure is the LiB<sub>3</sub>O<sub>5</sub>.</p>
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<p>Spectra of the frequency-doubled (<b>left</b>) and fundamental (<b>right</b>) VECSEL.</p>
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<p>The measured M<sup>2</sup> factor of the VECSEL.</p>
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<p>(<b>a</b>) Schematic of the 108 m distance UWOC system based on blue VECSEL. AOM in the picture means acousto-optic modulator; AWG in the picture means arbitrary waveform generator; PPM in the picture means pulse position modulation. (<b>b</b>) Transmitter of the UWOC system. (<b>c</b>) Underwater reflector. (<b>d</b>) Receiving equipment is avalanche photodiode (APD). (<b>e</b>) Underwater communication link and mixed-signal oscilloscope (MSO).</p>
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<p>(<b>a</b>) Schematic of acousto-optic Bragg modulation. RF in the picture means radio frequency. (<b>b</b>) Normalized signal modulation depth corresponding to pulse width.</p>
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<p>Eye diagrams of signals with frequencies of 10 MHz (<b>a</b>), 20 MHz (<b>b</b>), 50 MHz (<b>c</b>), and 100 MHz (<b>d</b>).</p>
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<p>Power requirements versus bandwidth requirements with on-off keying (OOK) and pulse position modulation (PPM).</p>
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<p>(<b>a</b>) Unfiltered 64 PPM signal. (<b>b</b>) Filtered and sampled 64 PPM signal.</p>
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<p>Relationship between bit error rate (BER) and received optical power for different orders of PPM at 10 MHz (<b>a</b>), 20 MHz (<b>b</b>), 50 MHz (<b>c</b>), and 100 MHz (<b>d</b>) time slot frequencies; FEC means forward error correction.</p>
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<p>Attenuation coefficient of the used 490 nm blue laser.</p>
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<p>Laser beam size at 24 m (<b>a</b>), 48 m (<b>b</b>) and 108 m (<b>c</b>). Signal eye diagram at 24 m (<b>d</b>), 48 m (<b>e</b>) and 108 m (<b>f</b>).</p>
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11 pages, 5060 KiB  
Article
Flexible Modulation of Perfect Vortex Beams by Combining Coherent Beams
by Bowang Shu, Yuqiu Zhang, Hongxiang Chang, Shiqing Tang, Jinyong Leng, Jiangming Xu and Pu Zhou
Photonics 2024, 11(4), 385; https://doi.org/10.3390/photonics11040385 - 18 Apr 2024
Viewed by 1074
Abstract
Perfect vortex beams (PVBs) possess the advantage of a stable light field distribution regardless of their topological charges, and thus they are extensively utilized in various applications, such as free-space optical communication, optical tweezers and laser processing. Herein, we report a new strategy [...] Read more.
Perfect vortex beams (PVBs) possess the advantage of a stable light field distribution regardless of their topological charges, and thus they are extensively utilized in various applications, such as free-space optical communication, optical tweezers and laser processing. Herein, we report a new strategy to generate and modulate PVBs using coherent beam combining (CBC) technology. Both piston phase and tilting phase controlling methods have been successfully employed, and the corresponding properties of the generated PVBs have been fully investigated. Moreover, the number and position of the gaps in fractional perfect vortex beams (FPVBs) could be precisely controlled, and the relationships between these modulated parameters and the performance of FPVBs are uncovered. These simulation analysis results demonstrate the potential for flexible modulation of PVBs or FPVBs in the CBC system, indicating promising prospects for coherent beam arrays (CBAs) in laser beam shaping and achieving high-power structured light. Full article
(This article belongs to the Section Lasers, Light Sources and Sensors)
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<p>Schematics of a CBC system for generation and modulation of PVBs or FPVBs. Inset: near-field amplitude distribution.</p>
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<p>The results of generated PVBs by employing a piston phase in a CBC system. (<b>a1</b>–<b>a3</b>) Far-field intensity distribution. Insets: near-field phase distribution in the CBA. (<b>b1–b3</b>) Far-field phase distribution of generated PVBs with varied topological charges of 1, 2 and 3.</p>
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<p>The mechanisms underlying generated PVBs by employing a piston phase in a CBC system. (<b>a1</b>) The generated BG beam as <span class="html-italic">l</span> = 1; (<b>a2</b>–<b>a4</b>) interceptive BG beams at filtering thresholds of 0.074, 0.062 and 0.051 m, respectively; (<b>a5</b>–<b>a7</b>) corresponding far-field intensity of PVBs as <span class="html-italic">l</span> = 1. (<b>b1</b>) The generated BG beam as <span class="html-italic">l</span> = 2; (<b>b2</b>–<b>b4</b>) interceptive BG beams at filtering thresholds of 0.068, 0.056 and 0.044 m, respectively; (<b>b5</b>–<b>b7</b>) corresponding far-field intensity of PVBs as <span class="html-italic">l</span> = 2. (<b>c1</b>) The generated BG beam as <span class="html-italic">l</span> = 3; (<b>c2</b>–<b>c4</b>) interceptive BG beams at filtering thresholds of 0.061, 0.048 and 0.037 m, respectively; (<b>c5</b>–<b>c7</b>) corresponding far-field intensity of PVBs as <span class="html-italic">l</span> = 3. (<b>d</b>) The relationships between the OAM mode purity and filtering thresholds. (<b>e</b>) The relationships between the diameter of PVBs and the filtering thresholds.</p>
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<p>PVBs with a controlled size by tuning the parameters of the aperture. (<b>a1</b>–<b>a3</b>) Near-field intensity distribution of a CBA with different numbers of apertures. (<b>b1</b>–<b>b3</b>) Corresponding far-field intensity distribution of the PVBs. (<b>c1</b>–<b>c3</b>) Near-field intensity distribution of a CBA with different radii of Gaussian-shaped beamlets. (<b>d1</b>–<b>d3</b>) Corresponding far-field intensity distribution of the PVBs.</p>
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<p>Modulation of FPVBs by employing a piston phase in a CBC system. (<b>a1</b>–<b>a5</b>) Near-field phase distribution; (<b>b1</b>–<b>b5</b>) far-field intensity distribution of an FPVB with a single gap. (<b>c1</b>–<b>c5</b>) Near-field phase distribution; (<b>d1</b>–<b>d5</b>) far-field intensity distribution of an FPVB with two gaps.</p>
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<p>The underlying mechanisms in FPVB modulation by a CBC system. (<b>a1</b>–<b>a4</b>) Far-field intensity distribution of FPVBs with different topological charges of <span class="html-italic">l</span> = 1.2, 1.4, 1.6 and 1.8, respectively. (<b>b1</b>–<b>b4</b>) Far-field intensity distribution of FPVBs formed by different numbers of apertures, <span class="html-italic">N</span> = 24, 36, 48 and 60, respectively. (<b>c</b>) The relationships between the number of apertures and the maximum available gaps. (<b>d1</b>,<b>d2</b>) the results of the far-field intensity distribution formed by 36 apertures. (<b>e1,e2</b>) the results of the far-field intensity distribution modulated by 96 apertures.</p>
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<p>The generation of PVBs by employing a tilting phase in a CBC system. (<b>a1</b>–<b>a3</b>) Near-field phase distribution; (<b>b1</b>–<b>b3</b>) far-field intensity and (<b>c1</b>–<b>c3</b>) phase distribution of PVBs with topological charges of <span class="html-italic">l</span> = 1, 2 and 3 at <span class="html-italic">r</span> = 150. (<b>d1</b>,<b>d2</b>) Near-field phase and (<b>e1</b>,<b>e2</b>) far-field intensity distribution of PVBs differing from periods <span class="html-italic">r</span>. (<b>f</b>) The relationship between the OAM mode purity and periods <span class="html-italic">r</span>.</p>
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<p>The relationship between the modulated tilting phase and the number of gaps. (<b>a1</b>–<b>a5</b>) Near-field phase distribution and (<b>b1–b5</b>) far-field intensity distribution of FPVBs with different gaps.</p>
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22 pages, 7787 KiB  
Article
RCEAU-Net: Cascade Multi-Scale Convolution and Attention-Mechanism-Based Network for Laser Beam Target Image Segmentation with Complex Background in Coal Mine
by Wenjuan Yang, Yanqun Wang, Xuhui Zhang, Le Zhu, Zhiteng Ren, Yang Ji, Long Li and Yanbin Xie
Sensors 2024, 24(8), 2552; https://doi.org/10.3390/s24082552 - 16 Apr 2024
Viewed by 767
Abstract
Accurate and reliable pose estimation of boom-type roadheaders is the key to the forming quality of the tunneling face in coal mines, which is of great importance to improve tunneling efficiency and ensure the safety of coal mine production. The multi-laser-beam target-based visual [...] Read more.
Accurate and reliable pose estimation of boom-type roadheaders is the key to the forming quality of the tunneling face in coal mines, which is of great importance to improve tunneling efficiency and ensure the safety of coal mine production. The multi-laser-beam target-based visual localization method is an effective way to realize accurate and reliable pose estimation of a roadheader body. However, the complex background interference in coal mines brings great challenges to the stable and accurate segmentation and extraction of laser beam features, which has become the main problem faced by the long-distance visual positioning method of underground equipment. In this paper, a semantic segmentation network for underground laser beams in coal mines, RCEAU-Net, is proposed based on U-Net. The network introduces residual connections in the convolution of the encoder and decoder parts, which effectively fuses the underlying feature information and improves the gradient circulation performance of the network. At the same time, by introducing cascade multi-scale convolution in the skipping connection section, which compensates for the lack of contextual semantic information in U-Net and improves the segmentation effect of the network model on tiny laser beams at long distance. Finally, the introduction of an efficient multi-scale attention module with cross-spatial learning in the encoder enhances the feature extraction capability of the network. Furthermore, the laser beam target dataset (LBTD) is constructed based on laser beam target images collected from several coal mines, and the proposed RCEAU-Net model is then tested and verified. The experimental results show that, compared with the original U-Net, RCEAU-Net can ensure the real-time performance of laser beam segmentation while increasing the Accuracy by 0.19%, Precision by 2.53%, Recall by 22.01%, and Intersection and Union Ratio by 8.48%, which can meet the requirements of multi-laser-beam feature segmentation and extraction under complex backgrounds in coal mines, so as to further ensure the accuracy and stability of long-distance visual positioning for boom-type roadheaders and ensure the safe production in the working face. Full article
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<p>The laser beam-based visual positioning system that was under industrial testing at the tunneling face and its collected laser beam image.</p>
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<p>The architecture of the U-Net network model.</p>
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<p>The architectures of the RCEAU-Net.</p>
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<p>The residual block. Here, two sets of BN, ReLU, and Conv 3 × 3 are used for feature extraction of the input feature, respectively, and an identity mapping of the initial feature to the final feature is performed in place of the convolutional blocks in the conventional U-Net network.</p>
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<p>The CMSC module. Here, three kinds of convolution kernels, Conv 5 × 5, Conv 3 × 3, and Conv 1 × 1, are used to build a cascade multi-scale convolution module to extract multi-scale feature information, and complete the fusion of feature maps through “Concatenation”, and finally use Conv 1 × 1 to restore the feature dimensions, so as to make up for the semantic gaps in the part of the jump connection.</p>
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<p>CA module. “C”, “H”, and “W” are the number of channels, height, and width of the feature maps, respectively. “X Avg Pool” refers to 1D horizontal global pooling, and “Y Avg Pool” means 1D vertical global pooling. “Re-weight” is the adjusted weight matrix.</p>
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<p>EMA module. “G” means grouping, “X Avg Pool” denotes the one-dimensional horizontal global pooling, and “Y Avg Pool” means one-dimensional vertical global pooling.</p>
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<p>The Laser beam target images. The bottom right area shows a local enlargement of the laser beam target in the original image.</p>
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<p>Laser beam image feature enhancement. “Origin” indicates the original image captured with the industrial camera. “Enhanced” indicates the enhanced image.</p>
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<p>The loss and accuracy curves of RCEAU-Net when trained on LBTD datasets. The black curve represents loss and the red curve represents accuracy.</p>
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<p>The segmentation effect of different models for laser beams.</p>
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<p>The feature refinement results.</p>
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<p>The 3D distribution of laser beam grey value, as shown in the lower right corner. The gray value of pixels close to the yellow region becomes larger, and the gray value of pixels close to the blue region becomes smaller.</p>
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<p>The center line fitting results of multi-laser beams.</p>
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3 pages, 385 KiB  
Abstract
Magnetic Field Sensors for Non-Invasive Current Monitoring in Wire-Bond-Less Power Modules
by Perla Malagò, Stefano Lumetti, Dominik Holzmann, Michael Ortner and Ali Roshanghias
Proceedings 2024, 97(1), 100; https://doi.org/10.3390/proceedings2024097100 - 27 Mar 2024
Viewed by 486
Abstract
A non-invasive implementation of a planar magnetoresistive sensor on top of copper interconnected power modules is proposed. This solution allows for the real-time monitoring of the electrical current flowing across the power modules. Anisotropic magnetoresistive (AMR) sensors made of Permalloy were designed through [...] Read more.
A non-invasive implementation of a planar magnetoresistive sensor on top of copper interconnected power modules is proposed. This solution allows for the real-time monitoring of the electrical current flowing across the power modules. Anisotropic magnetoresistive (AMR) sensors made of Permalloy were designed through finite-difference and finite-element simulations in the so-called barber-pole configuration and microfabricated via patterning by laser lithography and thin film deposition by electron-beam evaporation. Finally, the sensor performance was tested by measuring the magnetic field generated by the electrical current in a specific range of interest. Full article
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<p>(<b>a</b>) Top view of the PM sub-assembly together with the planar interconnects and magnetic field sensor. (<b>b</b>) ΔV measured for different values of <span class="html-italic">i</span> and <span class="html-italic">i<sub>s</sub></span>.</p>
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25 pages, 4495 KiB  
Review
Advances in Semiconductor Lasers Based on Parity–Time Symmetry
by Hongbo Sha, Yue Song, Yongyi Chen, Jishun Liu, Mengjie Shi, Zibo Wu, Hao Zhang, Li Qin, Lei Liang, Peng Jia, Cheng Qiu, Yuxin Lei, Yubing Wang, Yongqiang Ning, Guoqing Miao, Jinlong Zhang and Lijun Wang
Nanomaterials 2024, 14(7), 571; https://doi.org/10.3390/nano14070571 - 26 Mar 2024
Viewed by 1290
Abstract
Semiconductor lasers, characterized by their high efficiency, small size, low weight, rich wavelength options, and direct electrical drive, have found widespread application in many fields, including military defense, medical aesthetics, industrial processing, and aerospace. The mode characteristics of lasers directly affect their output [...] Read more.
Semiconductor lasers, characterized by their high efficiency, small size, low weight, rich wavelength options, and direct electrical drive, have found widespread application in many fields, including military defense, medical aesthetics, industrial processing, and aerospace. The mode characteristics of lasers directly affect their output performance, including output power, beam quality, and spectral linewidth. Therefore, semiconductor lasers with high output power and beam quality are at the forefront of international research in semiconductor laser science. The novel parity–time (PT) symmetry mode-control method provides the ability to selectively modulate longitudinal modes to improve the spectral characteristics of lasers. Recently, it has gathered much attention for transverse modulation, enabling the output of fundamental transverse modes and improving the beam quality of lasers. This study begins with the basic principles of PT symmetry and provides a detailed introduction to the technical solutions and recent developments in single-mode semiconductor lasers based on PT symmetry. We categorize the different modulation methods, analyze their structures, and highlight their performance characteristics. Finally, this paper summarizes the research progress in PT-symmetric lasers and provides prospects for future development. Full article
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<p>PT-symmetric optical structures. Periodically arranged 760 nm-wide sinusoidal-shaped combo structures are applied on top of an 800 nm-wide Si waveguide embedded inside SiO<sub>2</sub> to mimic parity–time optical potentials, in which imaginary part modulation is implemented with 14 nm Ge/24 nm Cr structures and 51 nm Si layers are for real part modulation. Reprinted with permission from Ref. [<a href="#B28-nanomaterials-14-00571" class="html-bibr">28</a>]. Copyright 2013, Springer Nature.</p>
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<p>Schematic of a Fabry–Perot cavity composed of dual gratings; M1 and M2 are PT-symmetric unidirectional gratings and non-reflective ends placed in the cavity outwards. Reprinted with permission from Ref. [<a href="#B54-nanomaterials-14-00571" class="html-bibr">54</a>]. Copyright 2013, Optical Society of America.</p>
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<p>Schematic of an electrically injected PT-symmetric laser structure. The waveguide layer consists of Al(x)GaAs, which has a refractive index of n ≈ 3.42. The quantum well is made up of GaAs and GaIn(x)As. Reprinted with permission from Ref. [<a href="#B26-nanomaterials-14-00571" class="html-bibr">26</a>]. Copyright 2020, Science Press.</p>
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<p>(<b>a</b>) Principle of PT-symmetric gratings, with symmetry planes of gratings (dashed lines) shifted by a quarter. (<b>b</b>) Schematic of a DFB laser structure with PT-symmetric grating. The waveguide layer consists of InP and the quantum well is made up of InGaAsP. Reprinted with permission from Ref. [<a href="#B45-nanomaterials-14-00571" class="html-bibr">45</a>]. Copyright 2021, De Gruyter.</p>
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<p>Scanning electron microscope image of PT-symmetric micro-ring laser. © The American Association for the Advancement of Science. Reprinted with permission from Ref. [<a href="#B25-nanomaterials-14-00571" class="html-bibr">25</a>]. Copyright 2014, The American Association for the Advancement of Science.</p>
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<p>(<b>a</b>) Schematic of the PT-symmetric circular Bragg laser. (<b>b</b>) Distribution of the refractive index in the radial direction, showing periodic modulation of both the real and imaginary parts of the refractive index, where <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>n</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math> is the average effective refractive index. <math display="inline"><semantics> <mrow> <mo>Δ</mo> <msub> <mrow> <mi>n</mi> </mrow> <mrow> <mi>r</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <mo>Δ</mo> <msub> <mrow> <mi>n</mi> </mrow> <mrow> <mi>i</mi> </mrow> </msub> </mrow> </semantics></math> are the modulation depths of the real and imaginary parts of the refractive index, respectively. Reprinted with permission from Ref. [<a href="#B59-nanomaterials-14-00571" class="html-bibr">59</a>]. Copyright 2014, Springer Nature.</p>
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<p>Laser spectra under (<b>a</b>,<b>b</b>) full and (<b>c</b>,<b>d</b>) half pumping. (<b>b</b>,<b>d</b>) are their corresponding laser spectra. Here, the pumping power is 23 μJ. The inset in (<b>d</b>) is the microscopic image of the sample. The width and length of the waveguide are 5 μm and 1 mm, respectively. Reprinted with permission from Ref. [<a href="#B61-nanomaterials-14-00571" class="html-bibr">61</a>]. Copyright 2016, John Wiley and Sons.</p>
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<p>Image of the CPAL manufactured on an InGaAsP/InP substrate. Reprinted with permission from Ref. [<a href="#B62-nanomaterials-14-00571" class="html-bibr">62</a>]. Copyright 2016, Springer Nature.</p>
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<p>(<b>a</b>) Heterostructure and (<b>b</b>) InAs quantum dot PT-symmetric coupled waveguide laser. Reprinted with permission from Ref. [<a href="#B75-nanomaterials-14-00571" class="html-bibr">75</a>]. Copyright 2019, John Wiley and Sons.</p>
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<p>Schematic and SEM of a biconical PT symmetric semiconductor laser. Reprinted with permission from Ref. [<a href="#B78-nanomaterials-14-00571" class="html-bibr">78</a>]. Copyright 2022, John Wiley and Sons.</p>
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<p>Schematic of a quasi-PT symmetric laser. The concept of quasi-PT symmetric edge-emitting lasers is realized with detuned coupled waveguide cavities. The propagation constant β decreases with increasing mode number, while the mode coupling is denoted by κ. By carefully selecting the cavity dimensions for isospectral engineering, resonant interactions between the second-order modes of the main potential and the fundamental modes of its lossy partners can be achieved, thus establishing quasi or modal PT symmetry. In this design, the electrical pumping of the main waveguide can act as a mode filter, enabling single-mode laser emission. Reprinted with permission from Ref. [<a href="#B79-nanomaterials-14-00571" class="html-bibr">79</a>]. Copyright 2023, Springer Nature.</p>
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<p>Experimental demonstration of PT-symmetry-breaking phase mode suppression. (<b>A</b>) Emission spectrum of a single resonator (radius 10 mm, ring width 500 nm, height 210 nm) when exposed to a peak pump power of 4.9 mW. (<b>B</b>) Corresponding intensity pattern in the ring observed from scattered light. (<b>C</b>) Emission spectrum obtained from a pair of uniformly pumped rings spaced 200 nm apart (4.9 mW + 4.9 mW). (<b>D</b>) Both rings have the same pattern intensity. (<b>E</b>) Single-mode spectrum under PT-symmetric conditions (0 mW + 4.9 mW pump). The SMSR exceeds 20 dB. (<b>F</b>) Lasing exclusively occurs in the active resonator. Reprinted with permission from Ref. [<a href="#B83-nanomaterials-14-00571" class="html-bibr">83</a>]. Copyright 2014, The American Association for the Advancement of Science.</p>
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<p>Schematic of a multimode single micro-ring and PT symmetric micro-rings. (<b>a</b>) In an isolated micro-ring resonator, multiple transverse and longitudinal modes can generate laser light simultaneously. (<b>b</b>) In a PT-symmetric arrangement, only one longitudinal mode with the lowest order transverse profile can emit laser light. Reprinted with permission from Ref. [<a href="#B24-nanomaterials-14-00571" class="html-bibr">24</a>]. Copyright 2016, John Wiley and Sons.</p>
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13 pages, 5332 KiB  
Article
Research on the Frequency Stabilization System of an External Cavity Diode Laser Based on Rubidium Atomic Modulation Transfer Spectroscopy Technology
by Yueyang Wu, Fangjun Qin, Zhichao Ding, Rui Xu and Dongyi Li
Photonics 2024, 11(4), 298; https://doi.org/10.3390/photonics11040298 - 25 Mar 2024
Cited by 1 | Viewed by 1075
Abstract
To achieve high-frequency stability on the external cavity diode laser (ECDL), a 780 nm ECDL serves as the seed light source, and its frequency is precisely locked to the saturated absorption peak of rubidium (Rb) atoms using modulation transfer spectroscopy (MTS) technology. For [...] Read more.
To achieve high-frequency stability on the external cavity diode laser (ECDL), a 780 nm ECDL serves as the seed light source, and its frequency is precisely locked to the saturated absorption peak of rubidium (Rb) atoms using modulation transfer spectroscopy (MTS) technology. For improving the performance of frequency locking, the scheme is designed to find the optimal operating conditions. Correlations between the frequency discrimination signal (FDS) and critical parameters, such as the temperature of the Rb cell, the power ratio of the probe and pump light, and the frequency and amplitude of the modulation and demodulation signals, are observed to attain the optimal conditions for frequency locking. To evaluate the performance of the frequency-stabilized 780 nm ECDL, a dual-beam heterodyne setup was constructed. Through this arrangement, the laser linewidth, approximately 65.4 kHz, is measured. Then, the frequency stability of the laser, quantified as low as 4.886 × 10−12 @32 s, is determined by measuring the beat-frequency signal with a frequency counter and calculating the Allan variance. Furthermore, using the realized frequency locking technology, the 780 nm ECDL can achieve long-term stabilization even after 25 h. The test results show the exceptional performance of the implemented frequency stabilization system for the 780 nm ECDL. Full article
(This article belongs to the Special Issue Technologies and Applications of Spectroscopy)
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<p>The overall scheme of the MTS frequency stabilization system. (<b>a</b>) PC. (<b>b</b>)Control box. (<b>c</b>) The commercial server. (<b>d</b>) The modem. (<b>e</b>) The dual-channel temperature control module. (<b>f</b>) The frequency-stabilized optical path.</p>
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<p>Adjusted SAS, MTS, and scanning signals.</p>
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<p>Normalized SAS signals corresponding to different temperatures. (<b>a</b>) 25 °C. (<b>b</b>) 30 °C. (<b>c</b>) 35 °C. (<b>d</b>) 40 °C. (<b>e</b>) 45 °C. (<b>f</b>) 50 °C.</p>
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<p>The peak-to-peak value of FDS corresponds to a different power of pump light. (<b>a</b>) 0.05 mW. (<b>b</b>) 0.075 mW. (<b>c</b>) 0.1 mW.</p>
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<p>The peak-to-peak value of FDS corresponds to the different frequency-stabilized light power.</p>
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<p>The peak-to-peak value of FDS corresponds to different modulation or demodulation voltage amplitudes. (<b>a</b>) The modulation voltage amplitudes. (<b>b</b>) The demodulation voltage amplitudes.</p>
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<p>The normalized peak-to-peak value and slope of FDS correspond to different modulation and demodulation frequencies. (<b>a</b>) <span class="html-italic">T</span><sub>3</sub>. (<b>b</b>) <span class="html-italic">T</span><sub>4</sub>.</p>
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<p>The beat frequency test of two lasers of the same model.</p>
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<p>The linewidth of the beat frequency signal.</p>
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<p>Beat frequency signal at 5000 s and laser stability. (<b>a</b>) Beat-frequency signal. (<b>b</b>) Allan variance.</p>
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<p>Laser frequency changes before and after frequency locking. (<b>a</b>) Before frequency locking. (<b>b</b>) After frequency locking.</p>
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11 pages, 3889 KiB  
Article
New Scheme of MEMS-Based LiDAR by Synchronized Dual-Laser Beams for Detection Range Enhancement
by Chien-Wei Huang, Chun-Nien Liu, Sheng-Chuan Mao, Wan-Shao Tsai, Zingway Pei, Charles W. Tu and Wood-Hi Cheng
Sensors 2024, 24(6), 1897; https://doi.org/10.3390/s24061897 - 15 Mar 2024
Viewed by 1181
Abstract
A new scheme presents MEMS-based LiDAR with synchronized dual-laser beams for detection range enhancement and precise point-cloud data without using higher laser power. The novel MEMS-based LiDAR module uses the principal laser light to build point-cloud data. In addition, an auxiliary laser light [...] Read more.
A new scheme presents MEMS-based LiDAR with synchronized dual-laser beams for detection range enhancement and precise point-cloud data without using higher laser power. The novel MEMS-based LiDAR module uses the principal laser light to build point-cloud data. In addition, an auxiliary laser light amplifies the single-noise ratio to enhance the detection range. This LiDAR module exhibits the field of view (FOV), angular resolution, and maximum detection distance of 45° (H) × 25° (V), 0.11° (H) × 0.11° (V), and 124 m, respectively. The maximum detection distance is enhanced by 16% from 107 m to 124 m with a laser power of 1 W and an additional auxiliary laser power of 0.355 W. Furthermore, the simulation results show that the maximum detection distance can be up to 300 m with laser power of 8 W and only 6 W if the auxiliary laser light of 2.84 W is used, which is 35.5% of the laser power. This result indicates that the synchronized dual-laser beams can achieve long detection distance and reduce laser power 30%, hence saving on the overall laser system costs. Therefore, the proposed LiDAR module can be applied for a long detection range in autonomous vehicles without requiring higher laser power if it utilizes an auxiliary laser light. Full article
(This article belongs to the Special Issue Multi-modal Sensor Fusion and 3D LiDARs for Vehicle Applications)
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<p>Block diagram of the MEMS-based LiDAR system with synchronized laser beams.</p>
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<p>A simple verification architecture of an optical path for the synchronized dual-laser beams. The path of the dashed line is the detection optical path from the main laser source, MEMS mirror, and receiver optics to APD. The path of the dash-dotted line is the enhanced signal optical path from the auxiliary laser source directly reaching the APD.</p>
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<p>The schematic of auxiliary light amplifies the reflected signal optically. The solid line represents the signal value, and the dotted line represents the threshold value.</p>
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<p>The time sequence of electrical trigger signal, primary and auxiliary lasers, and environmental noise obtained by an oscilloscope. To exceed the threshold, the power coupling of the main light and the auxiliary light must rely on an attenuator to adjust the power of the auxiliary light (A and B).</p>
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<p>The oscilloscope signal is directly from an APD on detecting reflected light in two types of LiDAR architecture: (<b>a</b>) without an auxiliary laser light and (<b>b</b>) with auxiliary laser illumination. The red solid line displays the value of the light signal, and the dotted line displays the value of the threshold.</p>
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<p>The point-cloud image from APD catches the received optical signal from the target (<b>a</b>) without an auxiliary laser light and (<b>b</b>) with auxiliary laser illumination. As seen by the image, under the identical detection effect, there are far more point clouds with the auxiliary light system turned on than without. Additionally, the edge features of the target object as a whole are made evident.</p>
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<p>The architecture of the hardware configuration for the MEMS-based LiDAR. Under the casing, the entire LiDAR structure covers the laser light source group, optical lens group, computer circuit board, electronic control circuit board, and power control circuit board. We set up every component grid using space optimization and visual route design.</p>
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<p>The method and analysis describe the FOV and angular resolution in MEMS-based LiDAR. Conduct the angular resolution test in the situation shown in (<b>a</b>). Configure the environment in compliance with the requirements of the standard test. Use trigonometric functions and point-cloud data to compute the angular resolution; (<b>b</b>) although the transmitted object’s actual size is equal to the proportionate relationship of the site size, users can utilize this information to estimate the approximate number of point clouds.</p>
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<p>The method and analysis description for the FOV and angular resolution in MEMS-based LiDAR: (<b>a</b>) is the optical image of the test environment; (<b>b</b>) is the point-cloud image without the auxiliary laser light; and (<b>c</b>) is the point-cloud image with the auxiliary laser light. The picture (<b>c</b>) shows more point clouds, project contours, and weak signals from objects farther behind.</p>
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<p>The maximum detection range is a function of the incident main laser power. The LiDAR presents the detection range by the line of dots when activating the auxiliary light system. The auxiliary light power is 35.5% of the leading laser power, and the squares line represents when the auxiliary light system is off. The detecting distance will be 16% farther when the auxiliary light system is active than when it is inactive.</p>
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