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0 pages, 2448 KiB  
Article
Collagen VI Deficiency Impairs Tendon Fibroblasts Mechanoresponse in Ullrich Congenital Muscular Dystrophy
by Vittoria Cenni, Patrizia Sabatelli, Alberto Di Martino, Luciano Merlini, Manuela Antoniel, Stefano Squarzoni, Simona Neri, Spartaco Santi, Samuele Metti, Paolo Bonaldo and Cesare Faldini
Cells 2024, 13(5), 378; https://doi.org/10.3390/cells13050378 - 22 Feb 2024
Cited by 1 | Viewed by 1515
Abstract
The pericellular matrix (PCM) is a specialized extracellular matrix that surrounds cells. Interactions with the PCM enable the cells to sense and respond to mechanical signals, triggering a proper adaptive response. Collagen VI is a component of muscle and tendon PCM. Mutations in [...] Read more.
The pericellular matrix (PCM) is a specialized extracellular matrix that surrounds cells. Interactions with the PCM enable the cells to sense and respond to mechanical signals, triggering a proper adaptive response. Collagen VI is a component of muscle and tendon PCM. Mutations in collagen VI genes cause a distinctive group of inherited skeletal muscle diseases, and Ullrich congenital muscular dystrophy (UCMD) is the most severe form. In addition to muscle weakness, UCMD patients show structural and functional changes of the tendon PCM. In this study, we investigated whether PCM alterations due to collagen VI mutations affect the response of tendon fibroblasts to mechanical stimulation. By taking advantage of human tendon cultures obtained from unaffected donors and from UCMD patients, we analyzed the morphological and functional properties of cellular mechanosensors. We found that the length of the primary cilia of UCMD cells was longer than that of controls. Unlike controls, in UCMD cells, both cilia prevalence and length were not recovered after mechanical stimulation. Accordingly, under the same experimental conditions, the activation of the Hedgehog signaling pathway, which is related to cilia activity, was impaired in UCMD cells. Finally, UCMD tendon cells exposed to mechanical stimuli showed altered focal adhesions, as well as impaired activation of Akt, ERK1/2, p38MAPK, and mechanoresponsive genes downstream of YAP. By exploring the response to mechanical stimulation, for the first time, our findings uncover novel unreported mechanistic aspects of the physiopathology of UCMD-derived tendon fibroblasts and point at a role for collagen VI in the modulation of mechanotransduction in tendons. Full article
(This article belongs to the Section Cell Motility and Adhesion)
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Figure 1

Figure 1
<p>Immunofluorescence and ultrastructural changes of collagen VI in UCMD tendon cultures. (<b>A</b>) Representative immunofluorescence for collagen VI (green) in TF cultures from control (CTRL) and UCMD (UCMD1-3) patients. Cells were grown to confluence and maintained 4 days in the presence of 0.25 mM L-ascorbic acid. In control cultures, collagen VI formed a dense extracellular network constituted by interconnected microfibrils (arrows). UCMD cultures displayed an altered arrangement of collagen VI networks, featuring dot-like deposits (arrowheads) in the ECM. In UCMD2 and UCMD3, the protein also accumulated in the cytoplasm (asterisks) of cells. (<b>B</b>) Representative image for double labeling with anti-collagen XII (upper panels, green) and collagen I (lower panels, red) in TF cultures, showing a coarse ECM arrangement (arrowheads) in UCMD cultures. In A and B, nuclei were stained with DAPI. Scale bar, 10 μm. (<b>C</b>) Transmission electron microscopy visualization of rotary shadowed replicas of proliferating TFs from control (CTRL), UCMD2, and UCMD3 patients, immunolabeled with anti-collagen VI and 5 nm-colloidal gold conjugated secondary antibody. In normal controls, colloidal gold particles associate with the globular domain of collagen VI tetramers, that, in turn, form microfilaments featuring “pearl necklace strands” (left upper panel, inset, white arrowheads), and complex webs. Other components of the ECM (upper right panel, white arrows), appear almost completely masked by the complex collagen VI webs. Note that in both UCMD TFs’ cultures, the few secreted collagen VI tetramers show irregular globular domains (left panels, white arrowheads): they form short microfilaments (right panels, white arrowheads), and the ECM, in general, due to the absence of collagen VI, has a smooth appearance (white arrows). Scale bar, 0.1 μm.</p>
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<p>PC organization and structure in control and UCMD tendon cultures. (<b>A</b>) Representative double immunofluorescence for Arl13b (red) and collagen VI (green) in control (CTRL) and UCMD (UCMD1-3) TFs. Arrows indicate the PC. Note the absence of collagen VI microfibrils in the proximity of the PC in all three UCMD cultures, opposite from the dense collagen VI network enveloping the PC in control cells. Nuclei were stained with DAPI. Scale bar, 5 μm. (<b>B</b>) Confocal imaging and 3D reconstruction of a single PC in control (CTRL) and collagen VI-deficient (UCMD) TFs, double-labeled with antibodies against collagen VI (green) and against acetylated α-tubulin (red), confirming the absence of collagen VI associated with the surface of the PC in UCMD TFs. Arrows indicate the extension of the cilium axoneme. Scale bar, 2 μm. (<b>C</b>) Scanning electron microscopy of normal (CTRL) and UCMD TFs, showing the presence of the PC (arrows) protruding from the cell surface. Higher magnifications on the right show the typical antenna-like structure of the PC. Scale bar of panels on the left 30 μm, and panels on the right 2 μm. (<b>D</b>) Representative immunofluorescence images of the PC in control (CTRL) and UCMD (UCMD1-3) TFs with an antibody against Arl13b (red), showing longer cilia in UCMD TFs. Nuclei were stained with DAPI. Scale bar, 2 μm. (<b>E</b>) Quantification of the PC length (upper panel) and PC prevalence (i.e., number of ciliated cells in percentage; lower panel) in cultured TFs from control (CTRL) and UCMD (UCMD1-3) patients, determined by immunofluorescence with an anti-Arl13b antibody. Measurements were performed with NIS AR 4.50 software, counting 100 cells for each culture. Significance was calculated by one-way ANOVA with Tukey’s multiple comparison test and was expressed between each UCMD and control TF under the same experimental conditions. * <span class="html-italic">p</span> &lt; 0.05; ns, not significant; <span class="html-italic">n</span> = 3.</p>
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<p>Modulation of PC and Hh signaling in control and UCMD tendon cultures under mechanical stress. (<b>A</b>) Representative immunofluorescence analysis of the PC in control (CTRL) and UCMD (UCMD1-3) TF cultures labeled with anti-Arl13b antibody (red), under unstrained condition (basal), after uniaxial strain (strain), and after a 3 h recovery from strain (recovery). Nuclei were stained with DAPI. Scale bar, 5 μm. (<b>B</b>) Quantification of PC prevalence (upper panel) and average PC length (lower panel) in control (CTRL) and UCMD TFs under the same conditions as in panel A. Statistical analysis by one-way ANOVA with Tukey’s multiple comparisons test. *, <span class="html-italic">p</span> &lt; 0.05; <b>**</b>, <span class="html-italic">p</span> &lt; 0.005; <span class="html-italic">n</span> = 3. (<b>C</b>) RT-qPCR analysis of GLI1 expression in control (CTRL) and UCMD TFs maintained in the above three conditions. RPLP0 served as the internal reference. Data are expressed as 2<sup>−ΔCt</sup> × 10<sup>5</sup> and presented as mean ± SD of at least three biological replicates. **, <span class="html-italic">p</span> &lt; 0.001; ns, not statistically significant; <span class="html-italic">n</span> = 4 control cultures, each condition; <span class="html-italic">n</span> = 3 UCMD cultures, each condition. (<b>D</b>) Representative immunofluorescence for GLI1 in control (CTRL) and UCMD TFs maintained in the above three conditions. Scale bar, 5 μm. (<b>E</b>) Quantification of the nuclear relative fluorescence intensity (F.I.) of GLI1 staining in control (CTRL) and UCMD TFs, based on GLI1 immunofluorescence as in D. For each culture, values were normalized on the respective basal condition. Measurements were performed with NIS AR 4.50 software, counting 70 cells for each culture. Statistical analysis by one-way ANOVA with Tukey’s multiple comparisons test. ** <span class="html-italic">p</span> &lt; 0.005, *** <span class="html-italic">p</span> &lt; 0.0001; ns, not significant; <span class="html-italic">n</span> = 3.</p>
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<p>Organization and activation of focal adhesions are impaired in UCMD tendon cultures during and after exposure to mechanical stress. (<b>A</b>,<b>B</b>) Magnification of confocal imaging of control (CTRL) and UCMD TFs under unstrained conditions (basal), at the end of mechanical stimulation (strain), and upon 3 h recovery from strain (recovery), following double labeling with fluorescent phalloidin (red) and with antibodies against A. talin (green) and B. phosphorylated FAK (pFAK, green). Nuclei were stained with DAPI. Scale bar, 10 µm. (<b>C</b>) 3D reconstruction of confocal imaging performed on control (CTRL) and UCMD TFs under unstrained conditions (basal), at the end of mechanical stimulation (strain), and upon 3 h recovery from strain (recovery), labeled with talin (green) and phalloidin (red). Nuclei were stained with DAPI. Scale bar, 5 µm. (<b>D</b>) Scanning electron microscopy of control (CTRL) and UCMD TF cultures under unstrained conditions (basal), at the end of mechanical stimulation (strain), and at the end of mechanical stimulation (recovery), showing an increased number of microvilli on the surface of UCMD cells in both stretched and recovery conditions. Scale bar 15 µm for low magnification, 5 µm inset. (<b>E</b>) Quantification of the number of microvilli per cell surface area in control and UCMD TFs in the above three conditions, based on scanning electron microscopy imaging as in D. Statistical analysis was performed by Student’s <span class="html-italic">t</span> test. **, <span class="html-italic">p</span> &lt; 0.05; <span class="html-italic">n</span> = 10 fields, each condition.</p>
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<p>Activation of signaling pathways downstream of focal adhesions is not properly restored in UCMD tendon cultures following recovery from mechanical stress. (<b>A</b>) Representative western blot analysis of the expression and the activation profile of talin and different protein kinases in TF cultures of control (CTRL) and UCMD (UCMD1-2) patients in the absence (−) or presence (+) of mechanical strain, as well as upon recovery for the indicated time (0, 0.5 and 3 h). Blots were incubated with antibodies against talin, phospho-Y397 FAK (P-FAK), total FAK, phospho-S473 Akt (P-Akt), total Akt, phospho-T202/Y204 ERK1/2 (P-ERK1/2), ERK2, phospho-T180/Y182 p38MAPK (P-p38MAPK), and total p38MAPK. GAPDH was used as a loading control. Molecular weight markers are reported on the right of the blots and are expressed in kDa. (<b>B</b>) Histograms of the relative densitometric quantifications normalized for GAPDH. ***, <span class="html-italic">p</span> &lt; 0.001; **, <span class="html-italic">p</span> &lt; 0.05; *, <span class="html-italic">p</span> &lt; 0.01; <span class="html-italic">n</span> = 3, each condition. (<b>C</b>) Representative immunofluorescence analysis of the subcellular localization of YAP (green) in control (CTRL) and UCMD TFs under unstrained conditions (basal), at the end of mechanical stimulation (strain), and upon 3 h recovery from strain (recovery). Upon stretching, YAP nuclear staining is displayed by control, but not by UCMD cells. Nuclei were stained with DAPI. Scale bar, 5 µm. (<b>D</b>) Quantification of the ratio of the mean fluorescence intensity of nuclear and cytoplasmic YAP, based on immunofluorescence analysis as in C. Data are presented as mean ± SEM. Statistical analysis by one-way ANOVA with Tukey’s multiple comparisons test. **, <span class="html-italic">p</span> &lt; 0.002; <span class="html-italic">n</span> = 30 measurement, each condition. (<b>E</b>) RT-qPCR analysis of CTGF and CYR61 mRNAs levels in control (CTRL) and UCMD TFs under unstrained conditions (basal), at the end of mechanical stimulation (strain), and upon 3 h recovery from strain (rec). Data are expressed as 2<sup>−ΔCt</sup> × 10<sup>5</sup> and presented as mean ± SD of at least three biological replicates. **, <span class="html-italic">p</span> &lt; 0.005; *, <span class="html-italic">p</span> &lt; 0.01; ns, not significant; <span class="html-italic">n</span> = 4 control cultures, each condition; <span class="html-italic">n</span> = 3 UCMD cultures, each condition.</p>
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<p>Mutations of collagen VI genes result in defective adaptation to mechanical strain. In normal TFs, following exposure to mechanical strain, at the PCM, the primary cilium (PC) and specific integrins interact with collagen VI, triggering the proper formation of focal adhesions (FA) and stress fibers, as well as the activation of a plethora of molecular pathways that lead to the translocation and activation of GLI1 and YAP. As a result, the upregulation of <span class="html-italic">GLI1</span> itself, <span class="html-italic">CYR61</span>, and <span class="html-italic">CTGF</span> is observed, with possible consequences on ECM remodeling and on the proper cellular adaptation to strain. The absence of a functional collagen VI, here observed on the right, impairs these mechanisms starting with an altered or even absent interaction between collagen VI and the PC, or with specific membrane receptors that result in a poor activation of the downstream molecular pathways. As a consequence, mechanoresponse and mechanotransduction are impaired, possibly leading to an impaired adaptation to stress. Green and red lines indicate active and impaired pathways, respectively.</p>
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25 pages, 1400 KiB  
Review
Hybrid Rice Production: A Worldwide Review of Floral Traits and Breeding Technology, with Special Emphasis on China
by Humera Ashraf, Fozia Ghouri, Faheem Shehzad Baloch, Muhammad Azhar Nadeem, Xuelin Fu and Muhammad Qasim Shahid
Plants 2024, 13(5), 578; https://doi.org/10.3390/plants13050578 - 21 Feb 2024
Cited by 5 | Viewed by 3345
Abstract
Rice is an important diet source for the majority of the world’s population, and meeting the growing need for rice requires significant improvements at the production level. Hybrid rice production has been a significant breakthrough in this regard, and the floral traits play [...] Read more.
Rice is an important diet source for the majority of the world’s population, and meeting the growing need for rice requires significant improvements at the production level. Hybrid rice production has been a significant breakthrough in this regard, and the floral traits play a major role in the development of hybrid rice. In grass species, rice has structural units called florets and spikelets and contains different floret organs such as lemma, palea, style length, anther, and stigma exsertion. These floral organs are crucial in enhancing rice production and uplifting rice cultivation at a broader level. Recent advances in breeding techniques also provide knowledge about different floral organs and how they can be improved by using biotechnological techniques for better production of rice. The rice flower holds immense significance and is the primary focal point for researchers working on rice molecular biology. Furthermore, the unique genetics of rice play a significant role in maintaining its floral structure. However, to improve rice varieties further, we need to identify the genomic regions through mapping of QTLs (quantitative trait loci) or by using GWAS (genome-wide association studies) and their validation should be performed by developing user-friendly molecular markers, such as Kompetitive allele-specific PCR (KASP). This review outlines the role of different floral traits and the benefits of using modern biotechnological approaches to improve hybrid rice production. It focuses on how floral traits are interrelated and their possible contribution to hybrid rice production to satisfy future rice demand. We discuss the significance of different floral traits, techniques, and breeding approaches in hybrid rice production. We provide a historical perspective of hybrid rice production and its current status and outline the challenges and opportunities in this field. Full article
(This article belongs to the Section Crop Physiology and Crop Production)
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<p>Schematic illustration of conventional and modern breeding strategies for hybrid rice production. GS (Genomic Selection), CMS (Cytoplasmic Male Sterile lines), GWAS (Genome-wide Association Study), gRNA (guide RNA), CRISPR (Clustered Regularly Interspaced Short Palindromic Repeats), MAS (Marker-assisted Selection).</p>
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<p>Rice floral and their related traits and their functions in hybrid rice production. DSE (double stigma exertion), SSE (single stigma exertion), NSE (no stigma exertion).</p>
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17 pages, 5844 KiB  
Article
Optical–Mechanical Integration Analysis and Validation of LiDAR Integrated Systems with a Small Field of View and High Repetition Frequency
by Lu Li, Kunming Xing, Ming Zhao, Bangxin Wang, Jianfeng Chen and Peng Zhuang
Photonics 2024, 11(2), 179; https://doi.org/10.3390/photonics11020179 - 16 Feb 2024
Cited by 1 | Viewed by 1115
Abstract
Integrated systems are facing complex and changing environments with the wide application of atmospheric LiDAR in civil, aerospace, and military fields. Traditional analysis methods employ optical software to evaluate the optical performance of integrated systems, and cannot comprehensively consider the influence of optical [...] Read more.
Integrated systems are facing complex and changing environments with the wide application of atmospheric LiDAR in civil, aerospace, and military fields. Traditional analysis methods employ optical software to evaluate the optical performance of integrated systems, and cannot comprehensively consider the influence of optical and mechanical coupling on the optical performance of the integrated system, resulting in the unsatisfactory accuracy of the analysis results. Optical–mechanical integration technology provides a promising solution to this problem. A small-field-of-view LiDAR system with high repetition frequency, low energy, and single-photon detection technology was taken as an example in this study, and the Zernike polynomial fitting algorithm was programmed to enable transmission between optical and mechanical data. Optical–mechanical integration technology was employed to obtain the optical parameters of the integrated system under a gravity load in the process of designing the optical–mechanical structure of the integrated system. The experimental validation results revealed that the optical–mechanical integration analysis of the divergence angle of the transmission unit resulted in an error of 2.586%. The focal length of the telescope increased by 89 μm, its field of view was 244 μrad, and the error of the detector target surface spot was 4.196%. The continuous day/night detection results showed that the system could accurately detect the temporal and spatial variations in clouds and aerosols. The inverted optical depths were experimentally compared with those obtained using a solar photometer. The average optical depth was 0.314, as detected using LiDAR, and 0.329, as detected by the sun photometer, with an average detection error of 4.559%. Therefore, optical–mechanical integration analysis can effectively improve the stability of the structure of highly integrated and complex optical systems. Full article
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<p>Optical–mechanical–thermal integrated analysis.</p>
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<p>LiDAR integrated systems: (<b>a</b>) schematic diagram and (<b>b</b>) internal structure diagram.</p>
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<p>Three-dimensional and finite element models of the LiDAR system: (<b>a</b>) three-dimensional simplified model; (<b>b</b>) finite element model.</p>
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<p>Establishment of local coordinate systems for each mirror of the transmitting unit: (<b>a</b>) transmitting unit; (<b>b</b>) receiving and aft optical units.</p>
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<p>Cloud diagram of reflecting mirror deformation under a gravity load: (<b>a</b>) transmission unit; (<b>b</b>) receiving and aft optical units.</p>
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<p>Dispersion spot of the transmission unit module: (<b>a</b>) no gravity load; (<b>b</b>) under a gravity load.</p>
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<p>Detector target surface spot in a ±125 μrad (half angle) field of view: (<b>a</b>) no gravity load; (<b>b</b>) under a gravity load.</p>
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<p>Detector target surface spot in a ±125 μrad (half angle) field of view: (<b>a</b>) no gravity load; (<b>b</b>) under a gravity load.</p>
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<p>Energy concentration of the 125 μrad (half angle) telescope system under a gravity load.</p>
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<p>(<b>a</b>) Optical–mechanical structure of the transmission unit and (<b>b</b>) detection optical path of divergence angle.</p>
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<p>Installation and testing of the receiving and aft optical unit optical–mechanical structures.</p>
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<p>Distance-corrected signals for (<b>a</b>) Parallel and (<b>b</b>) Vertical Palarization channels during the continuous detection period from 2 November 2020 to 5 November 2020.</p>
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<p>Inverted depolarization ratio profiles during continuous detection from 2 November 2020 to 5 November 2020.</p>
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<p>Comparison of inverted aerosol optical depths determined using LiDAR and the sun photometer on 7 November 2020.</p>
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19 pages, 4869 KiB  
Article
Design of an Internal Focusing Tube Lens for Optical Inspection Systems
by Daeje Jeon, Jungjin Park, Jaemyung Ryu and Hojong Choi
Appl. Sci. 2024, 14(4), 1518; https://doi.org/10.3390/app14041518 - 13 Feb 2024
Cited by 1 | Viewed by 971
Abstract
The numerical aperture (NA) of objective lens optical (inspection) systems has been increased to achieve higher resolution. However, the depth of focus decreases with an increase in the NA, and focusing becomes difficult. Therefore, the entire optical lens in currently developed optical inspection [...] Read more.
The numerical aperture (NA) of objective lens optical (inspection) systems has been increased to achieve higher resolution. However, the depth of focus decreases with an increase in the NA, and focusing becomes difficult. Therefore, the entire optical lens in currently developed optical inspection systems must be moved to focus within the depth of focus. To achieve a high resolution, many lenses are used in optical inspection systems, increasing the size and weight of the optical systems. To address this issue, a focus control group was placed on a tube lens that could adjust its focus based on the movement of the sample in front of the objective lens. Therefore, we developed a focus range increment to focus on the range of the optical inspection system. Using objective lenses with focal lengths of 30 and 60 mm and tube lenses with a focal length of 300 mm, optical systems for 10× and 5× inspection were constructed. In the designed optical systems, the weights of the objective lenses with focal lengths of 30 and 60 mm were calculated to be approximately 844 and 570 g, respectively. These values confirm that the weight of the moving group can be reduced. Full article
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<p>Airy disk [<a href="#B12-applsci-14-01518" class="html-bibr">12</a>].</p>
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<p>Schematic of a general microscope optical system.</p>
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<p>Sag value of the lens.</p>
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<p>Paraxial ray-tracing layout.</p>
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<p>Algorithm of the Gaussian bracket.</p>
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<p>Optical zoom system layout.</p>
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<p>Optical path diagram of the 10× optical system.</p>
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<p>Spot diagram of the 10× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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<p>Spot diagram of the 10× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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<p>Distortion aberration diagram of the 10× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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<p>Optical path diagram of the 5× optical system.</p>
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<p>Spot diagram of the 5× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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<p>Spot diagram of the 5× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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<p>Distortion aberration diagram of the 5× optical system when the sample moves (<b>a</b>) −0.36 mm from the reference point, (<b>b</b>) when the sample is located at the reference point, and (<b>c</b>) when the sample moves +0.36 mm.</p>
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15 pages, 3191 KiB  
Article
Renal Expression and Localization of the Receptor for (Pro)renin and Its Ligands in Rodent Models of Diabetes, Metabolic Syndrome, and Age-Dependent Focal and Segmental Glomerulosclerosis
by Carla Iacobini, Martina Vitale, Federica Sentinelli, Jonida Haxhi, Giuseppe Pugliese and Stefano Menini
Int. J. Mol. Sci. 2024, 25(4), 2217; https://doi.org/10.3390/ijms25042217 - 12 Feb 2024
Viewed by 956
Abstract
The (pro)renin receptor ((P)RR), a versatile protein found in various organs, including the kidney, is implicated in cardiometabolic conditions like diabetes, hypertension, and dyslipidemia, potentially contributing to organ damage. Importantly, changes in (pro)renin/(P)RR system localization during renal injury, a critical information base, remain [...] Read more.
The (pro)renin receptor ((P)RR), a versatile protein found in various organs, including the kidney, is implicated in cardiometabolic conditions like diabetes, hypertension, and dyslipidemia, potentially contributing to organ damage. Importantly, changes in (pro)renin/(P)RR system localization during renal injury, a critical information base, remain unexplored. This study investigates the expression and topographic localization of the full length (FL)-(P)RR, its ligands (renin and prorenin), and its target cyclooxygenase-2 and found that they are upregulated in three distinct animal models of renal injury. The protein expression of these targets, initially confined to specific tubular renal cell types in control animals, increases in renal injury models, extending to glomerular cells. (P)RR gene expression correlates with protein changes in a genetic model of focal and segmental glomerulosclerosis. However, in diabetic and high-fat-fed mice, (P)RR mRNA levels contradict FL-(P)RR immunoreactivity. Research on diabetic mice kidneys and human podocytes exposed to diabetic glucose levels suggests that this inconsistency may result from disrupted intracellular (P)RR processing, likely due to increased Munc18-1 interacting protein 3. It follows that changes in FL-(P)RR cellular content mechanisms are specific to renal disease etiology, emphasizing the need for consideration in future studies exploring this receptor’s involvement in renal damage of different origins. Full article
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<p>Immunostaining for full length-(pro)renin receptor (FL-(P)RR). Immunohistochemical (IHC) detection of FL-(P)RR and relative quantification of staining in renal specimens from control (Ctr), diabetic (Diab), and high fat diet (HFD) mice (<b>A</b>), and characteristics of the staining pattern in kidneys of Diab mice (<b>B</b>). IHC detection of FL-PRR, quantification, and immunostaining pattern in Wistar (WS) and Milan normotensive strain (MNS) rats at two and 9 months of age (<b>C</b>). Higher magnification images of IHC for FL-PRR in kidneys of Diab mice and 9-month-old MNS rats, counterstained or not with PAS, are shown in panels (<b>B</b>) and (<b>C</b>), respectively. Bars represent mean ± SD and each dot in (<b>A</b>,<b>C</b>) represents an individual animal. Arrows indicate positive cells in the tubular compartment, while arrowheads indicate glomerular cells with morphological features and topographical localization characteristic of podocytes. DCT, distal convoluted tubule; A, arteriole; CD, collecting duct; P, podocyte; M, mesangial cell; E, endothelial cell. Post hoc multiple comparison: *** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01, * <span class="html-italic">p</span> &lt; 0.05.</p>
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<p>Immunostaining for (pro)renin (total renin). Immunohistochemical (IHC) detection of renin without (<b>A</b>) and after (<b>B</b>) pretreatment with trypsin in sequential sections, and relative quantification of staining in renal specimens from control (Ctr), diabetic (Diab), and high fat diet (HFD) mice. The IHC detection of full length-(pro)renin receptor (FL-(P)RR) in a sequential section of the same kidney specimens, as depicted in panel B, reveals co-localization with total renin positivity at both tubular and glomerular levels (<b>C</b>). IHC detection of total renin and relative quantification of staining in renal specimens of Wistar (WS) and Milan normotensive strain (MNS) rats at two and 9 months of age (<b>D</b>). Bars represent mean ± SD and each dot in (<b>A</b>,<b>B</b>,<b>D</b>) represents an individual animal. Arrows indicate positive staining within juxtaglomerular areas, while arrowheads indicate glomerular cells with morphological features and topographical localization characteristic of podocytes. G, glomerulus. Post hoc multiple comparison: *** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01, * <span class="html-italic">p</span> &lt; 0.05.</p>
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<p>Immunostaining for cyclooxygenase-2 (COX-2). Immunohistochemical detection of COX-2 and relative quantification of staining in renal specimens from control (Ctr), diabetic (Diab), and high fat diet (HFD) mice (<b>A</b>), and in Wistar (WS) and Milan normotensive (MNS) rats at two and 9 months of age (<b>B</b>). Bars represent mean ± SD and each dot in (<b>A</b>,<b>B</b>) represents an individual animal. Arrows indicate positive staining of macula densa cells, while arrowheads indicate glomerular cells with morphological features and topographical localization characteristic of podocytes. G, glomerulus. Post hoc multiple comparison: *** <span class="html-italic">p</span> &lt; 0.001, * <span class="html-italic">p</span> &lt; 0.05.</p>
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<p>Gene expression of (pro)renin receptor ((P)RR) and associated factors governing its intracellular processing. (P)RR (<b>A</b>), furin (<b>B</b>), site-1 protease (S1P) (<b>C</b>), and Munc18-1 interacting protein 3 (Mint3) (<b>D</b>) mRNA levels in kidneys from control (Ctr), diabetic (Diab), and high fat diet (HFD) mice, and in Wistar (WS) and Milan normotensive strain (MNS) rats at 2 and 9 months of age. Bars represent mean ± SD and each dot in (<b>A</b>–<b>D</b>) represents an individual animal. Post hoc multiple comparison: *** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01, * <span class="html-italic">p</span> &lt; 0.05.</p>
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<p>Impact of HG on immunofluorescence (IF) staining and mRNA levels of (pro)renin receptor ((P)RR), gene expression of associated factors governing its intracellular processing, and soluble (s)(P)RR levels in the culture medium of podocytes. IF staining for full length (FL)-(P)RR with (<b>A</b>) and without (<b>B</b>) pretreatment with triton X-100, and mRNA levels of (P)RR (<b>C</b>), furin (<b>D</b>), site-1 protease (S1P) (<b>E</b>), and Munc18-1 interacting protein 3 (Mint3) (<b>F</b>), as well as s(P)RR levels in the culture medium (<b>G</b>) of podocytes exposed to high glucose (HG, 20 mM) vs. normal glucose (NG, 5.5 mM) for 72 h. Bars represent the mean ± SD, and each dot represents the mean of two (<b>C</b>–<b>F</b>) or three (<b>G</b>) individual technical replicates for each experimental condition. Post hoc multiple comparison: *** <span class="html-italic">p</span> &lt; 0.001, ** <span class="html-italic">p</span> &lt; 0.01.</p>
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15 pages, 12173 KiB  
Article
Deep Learning for Polarization Optical System Automated Design
by Haodong Shi, Ruihan Fan, Chunfeng He, Jiayu Wang, Shuai Yang, Miao Xu, Hongyu Sun, Yingchao Li and Qiang Fu
Photonics 2024, 11(2), 164; https://doi.org/10.3390/photonics11020164 - 8 Feb 2024
Viewed by 1169
Abstract
Aiming at the problem that traditional design methods make it difficult to control the polarization aberration distribution of optical systems quickly and accurately, this study proposes an automatic optimization design method for polarization optical systems based on deep learning. The unsupervised training model [...] Read more.
Aiming at the problem that traditional design methods make it difficult to control the polarization aberration distribution of optical systems quickly and accurately, this study proposes an automatic optimization design method for polarization optical systems based on deep learning. The unsupervised training model based on ray tracing and polarized ray tracing was constructed by learning the reference lens structural feature data from the optical lens library, and the generalization ability of the deep neural network model was improved to achieve the automatic optimization design of the polarized optical system. The design results show that the optical system structure optimized by the network model is close to the reference lens in the full field of view and the full spectrum and that the optical system structure can be designed for different focal length requirements. The success rate of 1 million groups of initial structures designed is better than 96.403%, and the polarization effect of the optical system is effectively controlled. The proposed deep learning approach to optical design provides a new solution for future complex optical systems and also provides an effective way to improve the design accuracy of special optical systems such as polarization optical systems. Full article
(This article belongs to the Section Optoelectronics and Optical Materials)
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<p>The learning process and design process of deep learning to design polarization optical systems.</p>
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<p>Comparison results of four groups of deep learning design lenses and reference lenses under different apertures while F is 14, 8, and 7. (<b>a</b>) Deep learning design lenses and reference lenses under different apertures while F is 14; (<b>b</b>) Deep learning design lenses and reference lenses under different apertures while F is 8 and HFOV is 0.5°; (<b>c</b>) Deep learning design lenses and reference lenses under different apertures while F is 8 and HFOV is 0.75°; (<b>d</b>) Deep learning design lenses and reference lenses under different apertures while F is 7.</p>
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<p>Comparison results of four groups of deep learning design lenses and reference lenses under different apertures while F is 6.4, 5, 4, and 2.8. (<b>a</b>) Deep learning design lenses and reference lenses under different apertures while F is 6.4; (<b>b</b>) Deep learning design lenses and reference lenses under different apertures while F is 5; (<b>c</b>) Deep learning design lenses and reference lenses under different apertures while F is 4; (<b>d</b>) Deep learning design lenses and reference lenses under different apertures while F is 2.8.</p>
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<p>Network model generalization ability test results. (<b>a</b>–<b>c</b>) Spot radius heat map of an optical system with different apertures and fields of view at different focal lengths; (<b>d</b>–<b>f</b>) Success ratio of optical system design with different apertures and fields of view at different focal lengths.</p>
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<p>Comparison results of four groups of polarization change deep learning design lenses polarization change and reference lenses under different apertures while Field is 14, 8, and 7 and FOV is 1, 0.75, and 0.5.</p>
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<p>Comparison results of four groups of polarization change deep learning design lenses and reference lenses under different apertures while Field is 6.4, 5, 4, and 2.8 and FOV is 2, 1.5, and 1.</p>
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<p>Comparison results of Stokes vector of deep learning design lenses and reference lenses under different apertures while Stokes is <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mn>0</mn> </msub> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mn>1</mn> </msub> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>S</mi> <mn>2</mn> </msub> </mrow> </semantics></math>.</p>
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11 pages, 4124 KiB  
Article
The SMILE Effect in the Beam Propagation Direction Affects the Beam Shaping of a Semiconductor Laser Bar Array
by Hongyou Zhang, Yu Hu, Shuihai Peng and Yong Liu
Photonics 2024, 11(2), 161; https://doi.org/10.3390/photonics11020161 - 7 Feb 2024
Viewed by 1090
Abstract
Near-field bending of a laser diode bar (i.e., the SMILE effect) degrades the laser beam brightness, adversely affecting optical coupling and beam shaping. Previous reports mainly focused on the two-dimensional near-field bending of a laser diode bar. However, the near-field bending of a [...] Read more.
Near-field bending of a laser diode bar (i.e., the SMILE effect) degrades the laser beam brightness, adversely affecting optical coupling and beam shaping. Previous reports mainly focused on the two-dimensional near-field bending of a laser diode bar. However, the near-field bending of a laser diode bar not only occurs in the laser bar growth direction, but also in the beam propagation direction. The present article proposes the three-dimensional near-field bending of a laser diode array, which is commonly known as the three-dimensional spatial SMILE effect. Through theoretical and simulated investigations, it has been found that a laser bar array not only deforms in the fast axis direction to cause the traditional two-dimensional SMILE effect but also experiences an additional deformation of approximately 2 μm in the laser emission direction simultaneously. Due to the SMILE effect in the beam propagation direction, not all emitters are aligned in a straight line, and some emitters experience defocusing during collimation. Consequently, there is an increase in the residual divergence angle and beam width, resulting in a degradation of the laser bar array’s beam quality. According to the theoretical calculations, ZEMAX simulations, and experimental results, for a FAC (fast axis collimation) with a focal length of 300 μm, the divergence angle of single emitter after collimating in the fast axis increases from 4.95 mrad to 6.46 mrad when the offsetting of the working distance between the incident beam waist and FAC lens increases from 0 μm to 2 μm. Full article
(This article belongs to the Special Issue Laser Beam Propagation and Control)
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<p>The force analysis diagram shows that the laser bar bonded on a heat sink experiences packaging-induced stress not only in the <span class="html-italic">X</span>-axis direction (slow axis direction) but also in the <span class="html-italic">Y</span>-axis direction (fast axis direction). The arrows indicate the direction of applied force.</p>
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<p>The simulation results of the near-field bending of a laser diode array are shown: (<b>a</b>) traditional two-dimensional near-field bending and (<b>b</b>) three-dimensional near-field bending of a laser diode array. Each black data point in the figures represents a single emitter of the laser diode array. In the three-dimensional near-field bending of a laser diode array, each emitter (black data point) is not only non-linear in the fast axis but also not aligned with the laser emission direction.</p>
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<p>The SMILE value in the beam propagation direction is 0.4 μm before bonding (as shown on the (<b>left</b>)) and 2.7 μm after bonding (as shown on the (<b>right</b>)). The abscissa axis represents the width of the laser bar array (cm bar), while the vertical coordinate represents the deformation of the laser diode array facet (SMILE effect in the beam propagation direction).</p>
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<p>The schematic diagram shows an individual FAC 300 lens from LIMO being attached to a conductive cooling device, where the position errors Δ<span class="html-italic">x</span>, Δ<span class="html-italic">y</span>, and Δ<span class="html-italic">z</span> represent the positional error, and <span class="html-italic">θx</span>, <span class="html-italic">θy</span>, and <span class="html-italic">θz</span> represent the angular errors of the FAC lens in its six degrees of freedom.</p>
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<p>Schematic diagram illustrating the transmission of a Gaussian beam through a thin lens.</p>
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<p>The 1/e<sup>2</sup> residual divergence angle changes as a function of the focal length <math display="inline"><semantics> <mi>F</mi> </semantics></math> of the FAC lens and the distance between the incident beam waist and FAC lens. FAC 300 refers to an FAC lens with a focal length of 300 μm.</p>
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<p>The near-field bending of a laser diode array in the beam propagation direction, as shown in the top view schematic diagram, affects the beam shaping of the laser diode array.</p>
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<p>The Gaussian beam of a single emitter in the fast axis direction of a COC device is simulated using ZEMAX after collimating with FAC 300.</p>
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<p>The Gaussian beam of a single emitter changes in the fast axis direction after collimating with FAC300 when the working distance that is offset increases from 0 μm to 5 μm.</p>
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<p>Beam shape of each emitter after FAC 300 collimating in fast axis direction, when assuming that the divergence angle is zero in the slow axis.</p>
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<p>(<b>a</b>) The testing results for beam width changes as a function of working distance offset. (<b>b</b>) The testing results of one COS device.</p>
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<p>Theoretical calculation, ZEMAX simulation, and experimental results showing that 1/e<sup>2</sup> residual divergence angle changes as a function of working distance offset.</p>
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10 pages, 721 KiB  
Article
Zebra Finch Females Avoided the Scent of Males with Greater Body Condition
by Luisa Amo and Isabel López-Rull
Birds 2024, 5(1), 127-136; https://doi.org/10.3390/birds5010009 - 6 Feb 2024
Viewed by 1358
Abstract
The role of chemical communication in the social relationships of birds is receiving growing attention, but our knowledge is still scarce compared to that of other taxa. Previous evidence suggests that chemical cues emitted by birds may carry information about their characteristics, which [...] Read more.
The role of chemical communication in the social relationships of birds is receiving growing attention, but our knowledge is still scarce compared to that of other taxa. Previous evidence suggests that chemical cues emitted by birds may carry information about their characteristics, which may be useful in the context of sexual selection. However, experimental studies are needed to investigate the role of bird chemical cues in signalling the quality of potential partners. We performed an experimental study aimed at disentangling whether the female Zebra Finches (Taeniopygia guttata), use chemical cues to assess the body condition of potential partners. We offered focal females (N = 28) the scent of two males differing in body condition (body mass/tarsus length ratio) (N = 28 scent donor males). Our results showed that females can assess the body condition of potential partners using olfaction. However, contrary to what should be expected in a mate choice context, females avoided the scent of males with greater body condition. Our results, therefore, suggest that, despite performing the study during the breeding period, social interactions may be mediating the avoidance of the scent of the male in better condition in this gregarious species, probably to avoid a conspecific competitor with better body condition. Full article
(This article belongs to the Special Issue Feature Papers of Birds 2022–2023)
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<p>Olfactometry chamber. The solid arrows indicate the direction of airflow within the chamber. Scent donor birds (black) were located at the farthest parts of the choice chambers inside cages. The focal bird (white) was introduced into the chamber and kept at the entrance for 5 min. After that time, the door was opened, and the focal bird was allowed to move to one of the two choice chambers.</p>
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<p>The first choice of focal Zebra Finch females, when exposed to the scent of two males, differed in quality in terms of body condition (body mass/tarsus length ratio). Most females (N = 20/28) chose the side of the chamber containing the scent of the male of worse quality (lower body condition).</p>
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15 pages, 3831 KiB  
Article
An Experimental Demonstration of 2D-Multiple-Input-Multiple-Output-Based Deep Learning for Optical Camera Communication
by Duy Tuan Anh Le, Huy Nguyen and Yeong Min Jang
Appl. Sci. 2024, 14(3), 1003; https://doi.org/10.3390/app14031003 - 24 Jan 2024
Cited by 1 | Viewed by 925
Abstract
Currently, radio frequency (RF) waveforms are widely used in wireless communication systems and are widely used in many fields to improve human quality of life. In Internet of Things (IoT) systems and satellite systems, the installation and deployment of wireless communication systems have [...] Read more.
Currently, radio frequency (RF) waveforms are widely used in wireless communication systems and are widely used in many fields to improve human quality of life. In Internet of Things (IoT) systems and satellite systems, the installation and deployment of wireless communication systems have become easier and offer many advantages compared to wired communication. However, high RF frequencies can have detrimental effects on the human body. Therefore, the visible light bandwidth is being researched and used as a replacement for RF in certain wireless communication systems. Several strategies have been explored: free-space optics, light fidelity, visible light communication, and optical camera communication. By leveraging time-domain on–off keying, this article presents a multiple-input-multiple-output (MIMO) modulation technique using a light-emitting diode (LED) array designed for IoT applications. The proposed scheme is versatile and suitable for both roller shutter and global shutter cameras commonly found on the market, including CCTV cameras commonly found in factories and buildings. By using deep learning for threshold prediction, the proposed scheme could achieve better performance compared to the traditional scheme. Despite the compact size of the LED array, the precise control of the exposure time, camera focal length, and channel encoding enabled the successful implementation of this scheme and supported four links at various positions within a communication distance of 22 m, taking into account the mobility effect (3 m/s). Full article
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<p>Reference architecture of 2D–MIMO technique based on a deep-learning neural network.</p>
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<p>Implementation results of the 2D MIMO scheme for an 8 × 8 LED matrix.</p>
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<p>System architecture of the deep-learning decoder for threshold prediction.</p>
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<p>BER curve for the optical OOK modulation.</p>
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<p>Spatial frame format in an LED array.</p>
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<p>Relationship between the focal length and communication distance.</p>
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<p>Quantized intensity profile of the LED matrix at 4 m with an exposure time of 300 µs.</p>
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<p>Setup scenario of proposed scheme with the LED matrix and webcam.</p>
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<p>Rx interface.</p>
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<p>BER performance of proposed system for an 8 × 8 LED array with different distances considering a velocity of 3 m/s with exposure time of 100 µs.</p>
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40 pages, 8730 KiB  
Review
Advancements in Fresnel Lens Technology across Diverse Solar Energy Applications: A Comprehensive Review
by Farhan Lafta Rashid, Mudhar A. Al-Obaidi, Ali Jafer Mahdi and Arman Ameen
Energies 2024, 17(3), 569; https://doi.org/10.3390/en17030569 - 24 Jan 2024
Cited by 1 | Viewed by 3042
Abstract
Concentration of solar energy may be obtained by reflection, refraction, or a combination of the two. The collectors of a reflection system are designed to concentrate the sun’s rays onto a photovoltaic cell or steam tube. Refractive lenses concentrate light by having it [...] Read more.
Concentration of solar energy may be obtained by reflection, refraction, or a combination of the two. The collectors of a reflection system are designed to concentrate the sun’s rays onto a photovoltaic cell or steam tube. Refractive lenses concentrate light by having it travel through the lens. The sun’s rays are partially reflected and then refracted via a hybrid technique. Hybrid focus techniques have the potential to maximize power output. Fresnel lenses are an efficient tool for concentrating solar energy, which may then be used in a variety of applications. Development of both imaging and non-imaging devices is occurring at this time. Larger acceptance angles, better concentration ratios with less volume and shorter focal length, greater optical efficiency, etc., are only some of the advantages of non-imaging systems over imaging ones. This study encompasses numerical, experimental, and numerical and experimental studies on the use of Fresnel lenses in various solar energy systems to present a comprehensive picture of current scientific achievements in this field. The framework, design criteria, progress, and difficulties are all dissected in detail. Accordingly, some recommendations for further studies are suggested. Full article
(This article belongs to the Special Issue Research on Energy, Environment, and Sustainable Development)
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<p>A hybrid distillation system in which (A) is the Fresnel lens, (B) are the batteries, (C) is the charge con-troller, (D) are the photovoltaic modules, (E) are the control system and electrical heater, (F) is the solar sensor, (G) are the tanks and pump, and (H) are the heat exchanger and focus system [<a href="#B30-energies-17-00569" class="html-bibr">30</a>].</p>
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<p>Top-level CAD design of V1 prototype solar front-end [<a href="#B31-energies-17-00569" class="html-bibr">31</a>].</p>
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<p>Version V2 desalination prototype top-level [<a href="#B31-energies-17-00569" class="html-bibr">31</a>].</p>
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<p>Picture of experimental setup [<a href="#B32-energies-17-00569" class="html-bibr">32</a>].</p>
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<p>System accumulation and hourly yields without Fresnel lens [<a href="#B32-energies-17-00569" class="html-bibr">32</a>].</p>
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<p>Two-eccentric tubular still working mechanism and energy transfer schematic map [<a href="#B33-energies-17-00569" class="html-bibr">33</a>].</p>
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<p>Solar still improved with a Fresnel lens [<a href="#B34-energies-17-00569" class="html-bibr">34</a>].</p>
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<p>July experiments: 1 and 2 cm depth productivity [<a href="#B37-energies-17-00569" class="html-bibr">37</a>].</p>
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<p>Hourly distilled water production [<a href="#B38-energies-17-00569" class="html-bibr">38</a>].</p>
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<p>Undeformed ZFL focus variations [<a href="#B45-energies-17-00569" class="html-bibr">45</a>].</p>
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<p>Schematic of experimental setup prototype [<a href="#B46-energies-17-00569" class="html-bibr">46</a>].</p>
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<p>Efficiency variations [<a href="#B47-energies-17-00569" class="html-bibr">47</a>].</p>
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<p>Experimental AFSCFL pictures [<a href="#B49-energies-17-00569" class="html-bibr">49</a>].</p>
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<p>Thermal performance of (<b>a</b>) AFSC and (<b>b</b>) AFSCFL constant-flow studies [<a href="#B49-energies-17-00569" class="html-bibr">49</a>].</p>
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<p>Geometrically modeled arrangement [<a href="#B51-energies-17-00569" class="html-bibr">51</a>].</p>
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<p>The soil temperature in the outer and inner hollow tubes varies with system length when I = 1000 W/m<sup>2</sup>, D<sub>o</sub> = 160 mm, and T<sub>in</sub> = 298 K [<a href="#B60-energies-17-00569" class="html-bibr">60</a>].</p>
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<p>Heat absorber cylinder temperature [<a href="#B63-energies-17-00569" class="html-bibr">63</a>].</p>
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<p>Solar thermal loop schematic [<a href="#B64-energies-17-00569" class="html-bibr">64</a>].</p>
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<p>Fresnel lens solar thermal energy storage [<a href="#B65-energies-17-00569" class="html-bibr">65</a>].</p>
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<p>Irradiance and temperature of the working medium vary with local time [<a href="#B66-energies-17-00569" class="html-bibr">66</a>].</p>
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<p>(<b>a</b>) Schematic and (<b>b</b>) photograph of fixed-focus Fresnel lens solar cooker [<a href="#B67-energies-17-00569" class="html-bibr">67</a>].</p>
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<p>Cavity receiver surface absorptivity affects fixed-focus optical performance. A Fresnel lens solar concentrator/conical cavity receiver [<a href="#B67-energies-17-00569" class="html-bibr">67</a>].</p>
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<p>Oil type and lens focal length affect cooking pot temperature (°C) [<a href="#B68-energies-17-00569" class="html-bibr">68</a>].</p>
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<p>Fresnel solar cooker heat efficiency [<a href="#B69-energies-17-00569" class="html-bibr">69</a>].</p>
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15 pages, 22815 KiB  
Article
Lightweight and High-Stiffness Metal Optical Systems Based on Additive Manufacturing
by Qiang Fu, Lei Yan, Shuanglong Tan, Yang Liu and Lingjie Wang
Micromachines 2024, 15(1), 128; https://doi.org/10.3390/mi15010128 - 12 Jan 2024
Viewed by 1202
Abstract
To build a long-wave infrared catadioptric optical system for deep space low-temperature target detection with a lightweight and wide field of view, this work conducted a study that encompasses a local cooling optical system, topology optimization-based metal mirror design, and additive manufacturing. First, [...] Read more.
To build a long-wave infrared catadioptric optical system for deep space low-temperature target detection with a lightweight and wide field of view, this work conducted a study that encompasses a local cooling optical system, topology optimization-based metal mirror design, and additive manufacturing. First, a compact catadioptric optical system with local cooling was designed. This system features a 55 mm aperture, a 110 mm focal length, and a 4-degree by 4-degree field of view. Secondly, we applied the principles of topology optimization to design the primary mirror assembly, the secondary mirror assembly, and the connecting baffle. The third and fourth modes achieved a resonance frequency of 1213.7 Hz. Then, we manufactured the mirror assemblies using additive manufacturing and single-point diamond turning, followed by the centering assembly method to complete the optical assembly. Lastly, we conducted performance testing on the system, with the test results revealing that the modulation transfer function (MTF) curves of the optical system reached the diffraction limit across the entire field of view. Remarkably, the system’s weight was reduced to a mere 96.04 g. The use of additive manufacturing proves to be an effective means of enhancing optical system performance. Full article
(This article belongs to the Section D:Materials and Processing)
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<p>A 2D diagram of the optical system.</p>
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<p>MTF curves of the optical system.</p>
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<p>Lattice structure.</p>
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<p>Equivalent analysis and design ideas of the mirror assembly.</p>
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<p>The diagram of the optical-mechanical system.</p>
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<p>Primary mirror assembly. (<b>a</b>) Front view; (<b>b</b>) Side view.</p>
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<p>The surface node displacement of the primary mirror under self-gravity. (<b>a</b>) Radial direction (X); (<b>b</b>) radial direction (Y); (<b>c</b>) axis direction (Z).</p>
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<p>Secondary mirror assembly.</p>
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<p>Shading baffle.</p>
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<p>The results of mode analysis. (<b>a</b>) First mode (708.3 Hz); (<b>b</b>) second mode (708.41 Hz); (<b>c</b>) third mode (1213.7 Hz); (<b>d</b>) fourth mode (1213.7 Hz).</p>
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<p>The results of system static analysis. (<b>a</b>) X radial direction; (<b>b</b>) Y radial direction; (<b>c</b>) Z radial direction.</p>
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<p>Primary mirror assembly by additive manufacturing. (<b>a</b>) Front view; (<b>b</b>) side view.</p>
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<p>Secondary mirror assembly by additive manufacturing. (<b>a</b>) Front view; (<b>b</b>) side view.</p>
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<p>Shading baffle by additive manufacturing.</p>
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<p>Primary mirror and surface shape data after SPDT. (<b>a</b>) Primary mirror; (<b>b</b>) surface quality.</p>
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<p>Secondary mirror and surface shape data after SPDT. (<b>a</b>) Secondary mirror; (<b>b</b>) surface quality.</p>
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<p>Primary mirror surface under high magnification camera.</p>
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<p>Primary mirror modified by Ni-P.</p>
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<p>Primary mirror and surface shape data after optical processing. (<b>a</b>) Primary mirror; (<b>b</b>) surface quality.</p>
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<p>Secondary mirror and surface shape data after optical processing. (<b>a</b>) Secondary mirror; (<b>b</b>) surface quality.</p>
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<p>Primary and secondary mirrors after gold-plating.</p>
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<p>The surface quality of the primary mirror after gold-plating.</p>
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<p>The surface quality of the secondary mirror after gold-plating.</p>
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<p>Centering alignment of primary and secondary mirror assembly. (<b>a</b>) Alignment worksite; (<b>b</b>) mirrors after centering.</p>
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<p>MTF test results for different FOVs. (<b>a</b>) The MTF curves of central FOV; (<b>b</b>) the MTF curves of 0.7 FOV; (<b>c</b>) the MTF curves of 1 FOV.</p>
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16 pages, 4358 KiB  
Article
Design of a Spaceborne, Compact, Off-Axis, Multi-Mirror Optical System Based on Freeform Surfaces
by Baohua Wang, Xiaoyong Wang, Huilin Jiang, Yuanyuan Wang, Chao Yang and Yao Meng
Photonics 2024, 11(1), 51; https://doi.org/10.3390/photonics11010051 - 3 Jan 2024
Cited by 1 | Viewed by 1300
Abstract
Based on the application requirements of high spectral resolutions, high spatial resolutions and wide swatches, a new-generation, high-performance, spaceborne, hyperspectral imaging spectrometer (NGHSI) with a spatial resolution of 15 m and a swatch of 90 km is proposed. The optical system of the [...] Read more.
Based on the application requirements of high spectral resolutions, high spatial resolutions and wide swatches, a new-generation, high-performance, spaceborne, hyperspectral imaging spectrometer (NGHSI) with a spatial resolution of 15 m and a swatch of 90 km is proposed. The optical system of the NGHSI has a focal length of 1128 mm, an F-number of three, a field of view (FOV) of 7.32° and a slit length of 144 mm. A new off-axis, multi-mirror telescope structure with intermediate images is put forward, which solves the design problem that realizes secondary imaging and good telecentricity at the same time. And a new off-axis lens-compensation Offner configuration is adopted to address the challenge of the high-fidelity design of spectral imaging systems with long slit lengths. The relationship between X-Y polynomials and aberration coefficients is analyzed, and the X-Y polynomial freeform surfaces are used to correct the off-axis aberrations. The design results show that the image quality of the telescope system is close to the diffraction limit. The smile, known as the spectral distortion along the line, and keystone, which is the magnification difference for different wavelengths, of the spectral imaging system are less than 1/10 pixel size. The complete optical system of the NGHSI, including the telescope system and the spectral imaging system, has excellent imaging quality and the layout is compact and reasonable, which realizes the miniaturization design. Full article
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<p>(<b>a</b>) Initial structure of coaxial multi-mirror optical system; (<b>b</b>) initial structure of off-axial multi-mirror optical system.</p>
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<p>(<b>a</b>) The classical Offner spectral imaging system; (<b>b</b>) the Wynne–Offner spectral imaging system; (<b>c</b>) the off-axis lens-compensated Offner spectral imaging system.</p>
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<p>Optical path diagram of the off-axis MMTS.</p>
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<p>(<b>a</b>) MTF curve of VNIR spectral band; (<b>b</b>) MTF curve of SWIR spectral band.</p>
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<p>(<b>a</b>) The sag of M<sub>3</sub>; (<b>b</b>) the sag deviation of M<sub>3</sub>; (<b>c</b>) the sag deviation of M<sub>3</sub> in the Y-direction.</p>
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<p>(<b>a</b>) The sag of M<sub>5</sub>; (<b>b</b>) the sag deviation of M<sub>5</sub>; (<b>c</b>) the sag deviation of M<sub>5</sub> in the Y-direction.</p>
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<p>(<b>a</b>) The VNIR off-axis lens-compensated Offner spectral imaging system; (<b>b</b>) the SWIR off-axis lens-compensated Offner spectral imaging system.</p>
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<p>(<b>a</b>) The smile in the VNIR spectral band; (<b>b</b>) the smile in the SWIR spectral band; (<b>c</b>) the keystone in the VNIR spectral band; (<b>d</b>) the keystone in the SWIR spectral band.</p>
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<p>The sag and deviation from base sphere of freeform surface of VNIR off-axis lens 1: (<b>a</b>) the sag; (<b>b</b>) the sag deviation; (<b>c</b>) the sag deviation in the Y-direction; the sag and deviation from base sphere of freeform surface of VNIR off-axis lens 2: (<b>d</b>) the sag; (<b>e</b>) the sag deviation; (<b>f</b>) the sag deviation in the Y-direction; the sag and deviation from base sphere of freeform surface of SWIR off-axis lens 1: (<b>g</b>) the sag; (<b>h</b>) the sag deviation; (<b>i</b>) the sag deviation in the Y-direction; the sag and deviation from base sphere of freeform surface of SWIR off-axis lens 2 (<b>j</b>) the sag; (<b>k</b>) the sag deviation; (<b>l</b>) the sag deviation in the Y-direction.</p>
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<p>Optical path diagram of the complete optical system.</p>
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<p>(<b>a</b>) MTF curve at 0.4 μm; (<b>b</b>) MTF curve at 1.0 μm; (<b>c</b>) MTF curve at 1.75 μm; (<b>d</b>) MTF curve at 2.5 μm.</p>
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<p>(<b>a</b>) MTF curve at 0.4 μm; (<b>b</b>) MTF curve at 1.0 μm; (<b>c</b>) MTF curve at 1.75 μm; (<b>d</b>) MTF curve at 2.5 μm.</p>
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15 pages, 5005 KiB  
Article
382 mW External-Cavity Frequency Doubling 461 nm Laser Based on Quasi-Phase Matching
by Yingxin Chen, Guodong Zhao, Wei Tan and Hong Chang
Photonics 2024, 11(1), 40; https://doi.org/10.3390/photonics11010040 - 30 Dec 2023
Viewed by 1309
Abstract
To rapidly improve strontium optical clocks, a high-power, high-efficiency, and high-beam-quality 461 nm laser is required. In blue lasers based on periodically poled KTiOPO4 crystals, the optical absorption in the crystals can induce thermal effects, which must be considered in the design [...] Read more.
To rapidly improve strontium optical clocks, a high-power, high-efficiency, and high-beam-quality 461 nm laser is required. In blue lasers based on periodically poled KTiOPO4 crystals, the optical absorption in the crystals can induce thermal effects, which must be considered in the design of high-efficiency external-cavity frequency doubling lasers. The interdependence between the absorption and the thermally induced quasi-phase mismatch was taken into account for the solution to the coupled wave equations. By incorporating multilayer crystal approximation, a theoretical model was developed to accurately determine the absorption of the frequency doubling laser. Based on experimental parameters, the temperature gradient in the crystal, the influence of the boundary temperature on the conversion efficiency, and the focal length of the thermal lens were simulated. Theoretical calculations were employed to optimize the parameters of the external-cavity frequency doubling experiment. In the experiment, in a bow-tie external cavity was demonstrated by pumping a 10 mm long periodically poled KTiOPO4 crystal with a 922 nm laser, a 461 nm laser with a maximum output power of 382 mW. The conversion efficiency of the incident fundamental laser was 66.2%. The M2 factor of the frequency doubling beam was approximately 1.4. Full article
(This article belongs to the Special Issue Narrow Linewidth Laser Sources and Their Applications)
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<p>Simulation of the dependence of the normalized SHG efficiency on the crystal oven temperature. This simulation did not include the thermal effects or absorption of the crystal.</p>
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<p>Simulation results of temperature distribution in a crystal. In these contour plots, blue represents low temperature and red represents high temperature. The laser beam was equaled to a parallel profile, but the laser intensity was distributed as a Gaussian function in the radial direction. (<b>a</b>) Temperature distribution over the entire <span class="html-italic">z</span>-axis section of the crystal; (<b>b</b>) temperature distribution in the crystal within the Gaussian diameter area of the laser.</p>
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<p>Simulation results of the relationship between the boundary temperature and the output power of the SHG laser. The red ball represents the results that take into account uneven absorption and temperature gradients in the crystal, and the blue line represents the results that do not consider crystal absorption. The dash line marks the maximum value of the blue solid line.</p>
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<p>External-cavity-enhanced conversion efficiency versus incident fundamental laser power for different intracavity linear losses. The linear loss values are marked above the solid curve.</p>
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<p>Schematic of experimental setup. DL pro: Toptica 922 nm ECDL seed laser; OI: 60dB optical isolator; TA: tapered amplifier; L1 and L2: mode matching lens; HR: high-reflectivity mirror for 922 nm; PD1 and PD2: photodiode; M1–M4: cavity mirrors; PZT: piezoelectric transducer; HV: high-voltage amplifier. The frequency of the seed laser was stabilized to the cavity mode via the lock-in method. The red solid line represents the 922 nm laser, and the blue solid line represents the 461 nm laser. The black solid line represents the fiber, and the black dash line represents the electronic cable.</p>
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<p>Normalized 461 nm output laser power versus crystal temperature. Due to the change in impedance matching and mode matching in the cavity, the curve was distorted compared with the sinc<sup>2</sup> function.</p>
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<p>Cavity modes of the fundamental laser. The incident fundamental laser power was maximum. (<b>a</b>) Reflected (upper red curve) and transmitted (down blue curve) cavity modes when scanning the cavity length. Mode-matching efficiency was calculated from the transmitted cavity modes. (<b>b</b>) Fundamental laser-reflected cavity mode in the scanning and locked states. Coupling efficiency was calculated from the reflected cavity mode.</p>
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<p>Measured and simulated 461 nm laser output power and cavity-enhanced SHG efficiency versus 922 nm laser input power. The measured results are shown as round and square spots, and the simulated results are shown as solid lines. In the experiment and simulation, the crystal temperature was set to 27.8 °C.</p>
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<p>The measured beam quality factors (M<sup>2</sup> value) of 461 nm output laser. Blue square spots and red round spots are the beam radii in the <span class="html-italic">X</span> and <span class="html-italic">Y</span> direction, respectively.</p>
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14 pages, 4375 KiB  
Article
Prolonged Fasting Induces Histological and Ultrastructural Changes in the Intestinal Mucosa That May Reduce Absorption and Revert after Enteral Refeeding
by Gonçalo Nunes, Marta Guimarães, Hélder Coelho, Ricardo Carregosa, Cátia Oliveira, Sofia S. Pereira, António Alves de Matos and Jorge Fonseca
Nutrients 2024, 16(1), 128; https://doi.org/10.3390/nu16010128 - 30 Dec 2023
Viewed by 1669
Abstract
Background: Malnutrition is usual in patients referred for endoscopic gastrostomy (PEG). Refeeding syndrome is rarely observed in PEG-fed patients, which could possibly be associated with reduced absorption induced by prolonged starvation. Objective: In patients submitted to PEG after a significant period of fasting, [...] Read more.
Background: Malnutrition is usual in patients referred for endoscopic gastrostomy (PEG). Refeeding syndrome is rarely observed in PEG-fed patients, which could possibly be associated with reduced absorption induced by prolonged starvation. Objective: In patients submitted to PEG after a significant period of fasting, the present study aims to: 1. evaluate the histological/ultrastructural initial changes in the intestinal mucosa, potentially associated with reduced absorption, and 2. assess if these changes could reverse with enteral refeeding. Methods: The present study is an observational, prospective, controlled study. Adult patients with ingestion below 50% of daily needs for at least one month and/or diagnosis of malnutrition were enrolled. Duodenal biopsies were taken at baseline and after 3–6 months of PEG feeding, which then underwent histological/ultrastructural analysis. Random healthy individuals were used as controls. Results: A total of 30 patients (16 men/14 women) aged 67.1 ± 13.5 years were included. Malnutrition was found in 40% of patients. Approximately 14 patients completed follow-up during both periods (46.7%). At baseline: duodenal mucosal atrophy was evident in three patients (10%); the median villi length (MVL) was 0.4 mm (0.25–0.6 mm), with it being shorter than the controls, which was 0.6 mm (0.4–0.7 mm) (p = 0.006); ultrastructural changes included focal shortening, bending, and disruption of enterocyte microvilli, the presence of citoplasmatic autophagic vacuoles, dilation and vesiculation of the smooth endoplasmic reticulum, and the presence of dilated intercellular spaces with basement membrane detachment. After refeeding, most patients displayed normal histology (92.9%) and increase MVL (p < 0.001), ultrastructural changes disappeared, and enterocytes resumed a normal appearance, although retaining scarce, small, dense bodies in apical regions from the evolution of previous autophagy. Conclusions: Prolonged fasting induces histological and ultrastructural changes in the intestinal mucosa that may reflect impaired absorption in the early post-PEG period. These changes were reverted after refeeding with enteral nutrition. Full article
(This article belongs to the Section Clinical Nutrition)
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<p>Patient flowchart: 30 patients were enrolled in the study and underwent PEG for long-term enteral nutrition after clinical, anthropometric, and laboratory evaluation. Duodenal biopsies were taken during the procedure for histologic and ultrastructure analysis. In total, 14 patients completed the study protocol, repeating duodenal mucosa assessment after 3–6 months of enteral refeeding. Normal healthy individuals submitted to upper GI endoscopy with duodenal biopsies were used as negative controls.</p>
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<p>Duodenal mucosa histology stained with hematoxylin and eosin (magnification 100×) exemplifying villi flattening measured at baseline in the patient (<b>A</b>) and control groups (<b>B</b>). The boxplot (<b>C</b>) displays both groups showing significant differences. * and circle are outliers markers.</p>
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<p>Duodenal mucosa histology stained with hematoxylin and eosin (magnification 100×) describing intestinal villi at T0 (<b>A</b>) and after refeeding (<b>B</b>). The boxplot (<b>C</b>) compares both study periods with significant differences. Circle are outliers markers.</p>
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<p>(<b>a</b>–<b>d</b>) Duodenal mucosa ultrastructure of patients undergoing prolonged fasting. Several degenerative changes can be observed namely: 1. microvilli shortening, bending, and disruption ((<b>b</b>,<b>c</b>)—arrows); 2. the presence of autophagic vacuoles, dense bodies ((<b>a</b>)—asterisks), vesiculation of the smooth endoplasmatic reticulum ((<b>b</b>)—asterisks), and heterogeneous mitochondria ((<b>c</b>)—asterisk); and 3. dilatation of intercellular spaces that were filled with medium-density granular material ((<b>d</b>)—asterisks).</p>
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<p>(<b>a</b>,<b>b</b>) Duodenal mucosa ultrastructure of the controls. The cells display a normal architecture: (<b>a</b>) microvilli (arrows) show a regular structure and (<b>b</b>) the cytoplasm (asterisks) has a conserved ultrastructure with normal organelles.</p>
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<p>(<b>a</b>,<b>b</b>) Duodenal mucosa ultrastructure of patients after enteral nutrition. Normal structure of microvilli and cytoplasm ((<b>a</b>)—asterisk) and the presence of residual bodies probably resulting from the autophagic activity ((<b>b</b>)—asterisks).</p>
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10 pages, 490 KiB  
Article
Long Stent Implantation on the Left Anterior Descending Coronary Artery at a Follow-Up of More Than Five Years
by Alessandro Sticchi, Concetta Tatali, Massimo Ferraro, Arif A. Khokhar, Alessandra Scoccia, Alberto Cereda, Marco Toselli, Francesco Gallo, Alessandra Laricchia, Antonio Mangieri, Francesco Grigioni, Gian Paolo Ussia, Francesco Giannini and Antonio Colombo
J. Clin. Med. 2024, 13(1), 210; https://doi.org/10.3390/jcm13010210 - 29 Dec 2023
Viewed by 1330
Abstract
Background: Stent implantation represents the standard of care in coronary intervention. While a short stent implanted on a focal lesion located on the left anterior descending artery (LAD) seems a reasonable alternative to an internal mammary implant, the same for long stents is [...] Read more.
Background: Stent implantation represents the standard of care in coronary intervention. While a short stent implanted on a focal lesion located on the left anterior descending artery (LAD) seems a reasonable alternative to an internal mammary implant, the same for long stents is still debated. Methods: We reported the long-term data of 531 consecutive patients who underwent Percutaneous Coronary Intervention (PCI) with long stents in two highly specialized centres. The main inclusion criteria were the implantation of stents longer than 30 mm on the LAD and a minimum follow-up (FU) of five years. The primary endpoint was mortality, and the secondary endpoints were any myocardial infarction (MI), target vessel and lesion revascularization (TVR and TLR, respectively), and stent thrombosis (ST) observed as definite, probable, or possible. Results: In this selected population with characteristics of complex PCI (99.1%), the long-term follow-up (mean 92.18 ± 35.5 months) estimates of all-cause death, cardiovascular death, and any myocardial infarction were 18.3%, 10.5%, and 9.3%, respectively. Both all-cause and cardiovascular deaths are significantly associated with three-vessel disease (HR 6.8; confidence of interval (CI) 95% 3.844–11.934; p < 0.001, and HR 4.7; CI 95% 2.265–9.835; p < 0.001, respectively). Target lesion (TLR) and target vessel revascularization (TVR) are associated with the presence of three-lesion disease on the LAD (HR 3.4; CI 95% 1.984–5.781; p < 0.001; HR 3.9 CI 95% 2.323–6.442; p < 0.001, respectively). Re-PCI for any cause occurred in 31.5% of patients and shows an increased risk for three-lesion stenting (HR 4.3; CI 95% 2.873–6.376; p < 0.001) and the treatment of bifurcation with two stents (HR 1.6; 95% CI 1.051–2.414; p = 0.028). Stent thrombosis rate at the 5-year FU was 4.4% (1.3% definite; 0.9% probable; 2.1% possible), including a 1.7% rate of very-late thrombosis. The stent length superior to 40 mm was not associated with poor outcomes (all-cause death p = 0.349; cardiovascular death p = 0.855; MI p = 0.691; re-PCI p = 0.234; TLR p = 0.805; TVR p = 0.087; ST p = 0.189). Conclusion: At an FU of longer than five years, patients treated with stents longer than 30 mm in their LAD showed acceptable procedural results but poor outcomes. Full article
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Graphical abstract
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<p>Patient inclusion flowchart for our study.</p>
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