[go: up one dir, main page]

 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

remove_circle_outline
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (450)

Search Parameters:
Keywords = focal length

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
13 pages, 5524 KiB  
Article
Simulation Analysis of Thermoacoustic Effect of CNT Film with Metasurface-Enhanced Acoustic Autofocusing
by Dalun Rong, Zhe Li, Qianshou Qi, Zhengnan Liu, Zhenhuan Zhou and Xinsheng Xu
Nanomaterials 2024, 14(18), 1481; https://doi.org/10.3390/nano14181481 - 11 Sep 2024
Viewed by 290
Abstract
This study introduces a novel thermoacoustic (TA) focusing system enhanced by Airy beam-based acoustic metasurfaces, significantly improving acoustic focusing and efficiency. The system integrates a TA emitter, fabricated from carbon nanotube (CNT) films, with a binary acoustic metasurface capable of generating quasi-Airy beams. [...] Read more.
This study introduces a novel thermoacoustic (TA) focusing system enhanced by Airy beam-based acoustic metasurfaces, significantly improving acoustic focusing and efficiency. The system integrates a TA emitter, fabricated from carbon nanotube (CNT) films, with a binary acoustic metasurface capable of generating quasi-Airy beams. Through finite element simulations, the system’s heat conduction, acoustic focusing, and self-healing properties were thoroughly analyzed. The results demonstrate that the system achieves superior sub-wavelength focusing, tunable focal length via frequency control, and robust self-healing, even in the presence of obstacles. These findings address current limitations in TA emitters and suggest broader applications in medical ultrasound and advanced technology. Full article
Show Figures

Figure 1

Figure 1
<p>Overview and phase modulation of the integrated thermoacoustic (TA) focusing system. (<b>a</b>) Schematic illustration of the integrated TA focusing system; (<b>b</b>) structure of the integrated system consisting of a TA emitter and a metasurface substrate; (<b>c</b>) pressure distribution <span class="html-italic">p</span><sub>0</sub> (blue line) of an ideal Airy beam and the approximate distribution p1 (red line); (<b>d</b>) phase and amplitude distribution of p1; (<b>e</b>) metasurface structure enabling phase-only modulation to approximating the quasi-Airy beam profile; (<b>f</b>–<b>h</b>) and an illustration of thermoacoustic wave propagation on a planar surface, a traditional spherical surface, and the integrated TA focusing system.</p>
Full article ">Figure 2
<p>Heat conduction and acoustic performance analysis of the integrated thermoacoustic (TA) system: (<b>a</b>) a section of the integrated TA focusing system; (<b>b</b>) the excitation current (black line) and temperature rise (red line) of the TA emitter; (<b>c</b>) variation in temperature rise (black line) and SPL (red line) with the material properties of film; (<b>d</b>) variation in thermal diffusion length with frequency; (<b>e</b>) temperature decay with distance, with the inset comparing thermal diffusion lengths in gap and the substrate; (<b>f</b>) sound intensity along the central axis (<span class="html-italic">r</span> = 0) under different heating powers; and (<b>g</b>) intensity contrast ratio <span class="html-italic">G</span> and acoustic intensity at the focal point as functions of input power.</p>
Full article ">Figure 3
<p>Parameters analysis (<span class="html-italic">r</span><sub>0</sub>, <span class="html-italic">w</span>) of the metasurface in the integrated thermoacoustic (TA) focusing system; (<b>a</b>) the sound intensity contrast ratio <span class="html-italic">G</span> at 1 MHz (<span class="html-italic">r</span><sub>0</sub> = 6.6 λ, <span class="html-italic">w</span> = 1.2 λ); (<b>b</b>–<b>e</b>) variation in the normalized intensity contrast ratio <span class="html-italic">G</span>, focal length <span class="html-italic">Z<sub>focus</sub></span>, full width at half-maximum (FWHM), and full length at half-maximum (FLHM) with the initial radial parameter <span class="html-italic">r</span><sub>0</sub> and scaling factor <span class="html-italic">w</span> of the metasurface. (<b>f</b>,<b>g</b>) Normalized intensity contrast ratio <span class="html-italic">G</span> along the axial direction (<span class="html-italic">r</span> = 0) and along the radial direction (<span class="html-italic">Z</span> = 41.6 λ).</p>
Full article ">Figure 4
<p>Impact of frequency on focusing characteristics in the thermoacoustic (TA)-integrated system: (<b>a</b>,<b>b</b>) intensity contrast ratio <span class="html-italic">G</span> and focal length <span class="html-italic">Z</span><sub>focus</sub> across a broad frequency range (0.88 MHz to 1.09 MHz); (<b>c</b>,<b>d</b>) variation in the full width at half-maximum (FWHM) and full length at half-maximum (FLHM) with the frequency; and (<b>e</b>–<b>h</b>) normalized acoustic intensity distributions at frequencies of 0.88 MHz, 0.94 MHz, 1.00 MHz, and 1.06 MHz.</p>
Full article ">Figure 5
<p>Self-healing focusing of the thermoacoustic (TA)-integrated system in the presence of obstacles: (<b>a</b>) schematic illustration of the obstacle placement; (<b>b</b>–<b>d</b>) effects of different obstacle shapes (oval, circular, and rectangular) on the intensity contrast ratio <span class="html-italic">G</span> at the focal point; (<b>e</b>–<b>h</b>) impact of obstacle size on the self-healing capability of the system; and (<b>i</b>) self-healing focusing in the presence of array-like obstacles.</p>
Full article ">
23 pages, 21056 KiB  
Article
Development and Application of Unmanned Aerial High-Resolution Convex Grating Dispersion Hyperspectral Imager
by Qingsheng Xue, Xinyu Gao, Fengqin Lu, Jun Ma, Junhong Song and Jinfeng Xu
Sensors 2024, 24(17), 5812; https://doi.org/10.3390/s24175812 - 7 Sep 2024
Viewed by 300
Abstract
This study presents the design and development of a high-resolution convex grating dispersion hyperspectral imaging system tailored for unmanned aerial vehicle (UAV) remote sensing applications. The system operates within a spectral range of 400 to 1000 nm, encompassing over 150 channels, and achieves [...] Read more.
This study presents the design and development of a high-resolution convex grating dispersion hyperspectral imaging system tailored for unmanned aerial vehicle (UAV) remote sensing applications. The system operates within a spectral range of 400 to 1000 nm, encompassing over 150 channels, and achieves an average spectral resolution of less than 4 nm. It features a field of view of 30°, a focal length of 20 mm, a compact volume of only 200 mm × 167 mm × 78 mm, and a total weight of less than 1.5 kg. Based on the design specifications, the system was meticulously adjusted, calibrated, and tested. Additionally, custom software for the hyperspectral system was independently developed to facilitate functions such as control parameter adjustments, real-time display, and data preprocessing of the hyperspectral camera. Subsequently, the prototype was integrated onto a drone for remote sensing observations of Spartina alterniflora at Yangkou Beach in Shouguang City, Shandong Province. Various algorithms were employed for data classification and comparison, with support vector machine (SVM) and neural network algorithms demonstrating superior classification accuracy. The experimental results indicate that the UAV-based hyperspectral imaging system exhibits high imaging quality, minimal distortion, excellent resolution, an expansive camera field of view, a broad detection range, high experimental efficiency, and remarkable capabilities for remote sensing detection. Full article
(This article belongs to the Section Remote Sensors)
Show Figures

Figure 1

Figure 1
<p>Optical structure of the front telescope system.</p>
Full article ">Figure 2
<p>Distribution of point columns on the image plane of the telescope system.</p>
Full article ">Figure 3
<p>Optical transfer function curve of the front telescope system.</p>
Full article ">Figure 4
<p>Optical structure of Offner spectral imaging system.</p>
Full article ">Figure 5
<p>MTF curves for different wavelengths of Offner spectral imaging system: (<b>a</b>) 400 nm; (<b>b</b>) 700 nm; (<b>c</b>) 1000 nm.</p>
Full article ">Figure 5 Cont.
<p>MTF curves for different wavelengths of Offner spectral imaging system: (<b>a</b>) 400 nm; (<b>b</b>) 700 nm; (<b>c</b>) 1000 nm.</p>
Full article ">Figure 6
<p>Curve of RMS radius versus wavelength for Offner spectral imaging system.</p>
Full article ">Figure 7
<p>Map of light imprints on the image plane of Offner spectral imaging system.</p>
Full article ">Figure 8
<p>Spectral bending at different wavelengths of Offner spectral imaging system.</p>
Full article ">Figure 9
<p>Spectral band bending for different fields of view of Offner spectral imaging system.</p>
Full article ">Figure 10
<p>System-wide optical structure of the hyperspectral imager.</p>
Full article ">Figure 11
<p>System-wide optical transfer function curve of hyperspectral imager.</p>
Full article ">Figure 12
<p>Overall mechanical structure of the hyperspectral prototype.</p>
Full article ">Figure 13
<p>Results of Gaussian fitting of some characteristic peaks: (<b>a</b>) 696.54 nm wavelength characteristic peak fitting result; (<b>b</b>) 738.40 nm wavelength characteristic peak fitting result; (<b>c</b>) 763.51 nm wavelength characteristic peak fitting result; (<b>d</b>) 772.40 nm wavelength characteristic peak fitting result; (<b>e</b>) 794.82 nm wavelength characteristic peak fitting result; (<b>f</b>) 912.30 nm wavelength characteristic peak fitting result.</p>
Full article ">Figure 14
<p>Hg lamp calibration fitting results.</p>
Full article ">Figure 15
<p>Overall functional block diagram of hyperspectral control software system.</p>
Full article ">Figure 16
<p>Screenshot of Software System Operation Test.</p>
Full article ">Figure 17
<p>Hyperspectral Imager System Outdoor Rotary Scanning Experiment.</p>
Full article ">Figure 18
<p>Monochromatic images at different wavelength bands from the outdoor push-scan of the hyperspectral imaging system: (<b>a</b>) monochromatic image in the 500 nm wavelength band; (<b>b</b>) monochromatic image in the 600 nm wavelength band; (<b>c</b>) monochromatic image in the 700 nm wavelength band; (<b>d</b>) monochromatic image in the 800 nm wavelength band.</p>
Full article ">Figure 18 Cont.
<p>Monochromatic images at different wavelength bands from the outdoor push-scan of the hyperspectral imaging system: (<b>a</b>) monochromatic image in the 500 nm wavelength band; (<b>b</b>) monochromatic image in the 600 nm wavelength band; (<b>c</b>) monochromatic image in the 700 nm wavelength band; (<b>d</b>) monochromatic image in the 800 nm wavelength band.</p>
Full article ">Figure 19
<p>Spectral intensity curves of roofs, walls, and green trees.</p>
Full article ">Figure 20
<p>Components of an unmanned airborne hyperspectral remote sensing system.</p>
Full article ">Figure 21
<p>Photo of the distribution area of <span class="html-italic">Spartina alterniflora</span> at Yangkou Beach.</p>
Full article ">Figure 22
<p>Monochromatic images of <span class="html-italic">Spartina alterniflora</span> captured by unmanned aerial vehicle hyperspectral system in different frequency bands: (<b>a</b>) monochromatic image in the 560 nm wavelength band; (<b>b</b>) monochromatic image in the 600 nm wavelength band; (<b>c</b>) monochromatic image in the 650 nm wavelength band; (<b>d</b>) monochromatic image in the 700 nm wavelength band; (<b>e</b>) monochromatic image in the 750 band; (<b>f</b>) monochromatic image in the 800 nm wavelength band; (<b>g</b>) monochromatic image in the 850 nm wavelength band.</p>
Full article ">Figure 22 Cont.
<p>Monochromatic images of <span class="html-italic">Spartina alterniflora</span> captured by unmanned aerial vehicle hyperspectral system in different frequency bands: (<b>a</b>) monochromatic image in the 560 nm wavelength band; (<b>b</b>) monochromatic image in the 600 nm wavelength band; (<b>c</b>) monochromatic image in the 650 nm wavelength band; (<b>d</b>) monochromatic image in the 700 nm wavelength band; (<b>e</b>) monochromatic image in the 750 band; (<b>f</b>) monochromatic image in the 800 nm wavelength band; (<b>g</b>) monochromatic image in the 850 nm wavelength band.</p>
Full article ">Figure 23
<p>Spectral curves of <span class="html-italic">Spartina alterniflora</span> Loisel, water, and mudflat.</p>
Full article ">Figure 24
<p>Classification results of hyperspectral data of <span class="html-italic">Spartina alterniflora</span> using different classification algorithms; among them, green represents <span class="html-italic">Spartina alterniflora</span>, light blue represents water area, and dark blue represents mudflat. (<b>a</b>) SAM classification results; (<b>b</b>) SID classification results l; (<b>c</b>) SVM classification results; (<b>d</b>) BPNN classification results.</p>
Full article ">
17 pages, 5451 KiB  
Article
Comparative Morphology of Skeletal Development in Homo sapiens and Raja asterias: Divergent Stiffening Patterns Due to Different Matrix Calcification Processes
by Ugo E. Pazzaglia, Piero A. Zecca, Genciana Terova, Fabrizio Serena, Cecilia Mancusi, Giovanni Raimondi, Guido Zarattini, Mario Raspanti and Marcella Reguzzoni
Animals 2024, 14(17), 2575; https://doi.org/10.3390/ani14172575 - 4 Sep 2024
Viewed by 234
Abstract
Before calcification begins, the early embryonic and fetal skeletal development of both mammalian Homo sapiens and the chondrichthyan fish Raja asterias consists exclusively of cartilage. This cartilage is formed and shaped through processes involving tissue segmentation and the frequency, distribution, and orientation of [...] Read more.
Before calcification begins, the early embryonic and fetal skeletal development of both mammalian Homo sapiens and the chondrichthyan fish Raja asterias consists exclusively of cartilage. This cartilage is formed and shaped through processes involving tissue segmentation and the frequency, distribution, and orientation of chondrocyte mitoses. In the subsequent developmental phase, mineral deposition in the cartilage matrix conditions the development further. The stiffness and structural layout of the mineralized cartilage have a significant impact on the shape of the anlagen (early formative structure of a tissue, a scaffold on which the new bone is formed) and the mechanical properties of the skeletal segments. The fundamental difference between the two studied species lies in how calcified cartilage serves as a scaffold for osteoblasts to deposit bone matrix, which is then remodeled. In contrast, chondrichthyans retain the calcified cartilage as the definitive skeletal structure. This study documents the distinct mineral deposition pattern in the cartilage of the chondrichthyan R. asterias, in which calcification progresses with the formation of focal calcification nuclei or “tesserae”. These are arranged on the flat surface of the endo-skeleton (crustal pattern) or aligned in columns (catenated pattern) in the radials of the appendicular skeleton. This anatomical structure is well adapted to meet the mechanical requirements of locomotion in the water column. Conversely, in terrestrial mammals, endochondral ossification (associated with the remodeling of the calcified matrix) provides limb bones with the necessary stiffness to withstand the strong bending and twisting stresses of terrestrial locomotion. In this study, radiographs of marine mammals (reproduced from previously published studies) document how the endochondral ossification in dolphin flippers adapts to the mechanical demands of aquatic locomotion. This adaptation includes the reduction in the length of the stylopodium and zeugopodium and an increase in the number of elements in the autopodium’s central rays. Full article
(This article belongs to the Section Aquatic Animals)
Show Figures

Figure 1

Figure 1
<p>Histology of the autopodial cartilage anlagen growth of <span class="html-italic">Homo sapiens</span> (hematoxylin–eosin, dec. sections). (<b>A</b>) Mitotic chondrocyte phase with dissolution of the nuclear membrane, doubling of the chromosomes and attachment to the spindle (prophase and metaphase). The red line shows the axis of the mitotic spindle. (<b>B</b>) Migration of the doubled chromosomes towards the spindle poles (anaphase). The red line shows the axis of the mitotic spindle. (<b>C</b>) Duplicated chondrocytes still in a single lacuna. The red line shows the axis of the duplicated chondrocytes. (<b>D</b>) Paired chondrocytes have formed their own lacunae, separated by matrix septa of increasing thickness. The red line shows the axis of the recently duplicated chondrocytes that have formed their own lacunae.</p>
Full article ">Figure 2
<p>Histology of the fetal autopodium of <span class="html-italic">Homo sapiens</span>. (<b>A</b>,<b>B</b>) (hematoxylin–eosin, dec. section) Form of the autopodium elements, with incipient mineral deposition in the middle sector of the metacarpals, not yet initiated in the short carpal bone anlagen and in the epiphyses. (<b>C</b>) (Alcian-blue, dec. section) Initial phase of mineral deposition with swelling of the chondrocytes (usually referred to as hypertrophy). At this stage, there are no signs of epiphyseal calcifying centers forming. (<b>D</b>) (Von Kossa-neutral red, un-dec. section) Mineral deposits in the cartilage matrix between the swollen chondrocytes and early mineral deposits in the periosteal bone envelope.</p>
Full article ">Figure 3
<p>Histology and primary calcified cartilage matrix resorption in <span class="html-italic">Homo sapiens</span> autopodium metacarpals. (<b>A</b>) (hematoxylin–eosin, dec. section) Swollen chondrocytes of the central anlage zone with matrix more densely stained by hematoxylin where mineral deposition occurs. Initial formation of the bone periosteal sleeve (red arrow). (<b>B</b>) (hematoxylin–eosin, dec. section) Vascular invasion and reabsorption of calcified cartilage matrix in the central zone of the anlage; the upper and lower sectors retain the denser colored matrix. Increased thickness of the bone periosteal sleeve (red arrow). (<b>C</b>) (hematoxylin–eosin, dec. section, bar = 100 μm) Advanced vascular invasion and calcified matrix resorption in the central zone of the anlage. (<b>D</b>) (Von Kossa neutral red, un-dec. section, bar = 100 μm) Residual calcified cartilage matrix of the central zone and first cortical bone layer of the diaphysis. (<b>E</b>) (hematoxylin–eosin, dec. section) Bone matrix (*) of the trabecula, resorbing two osteocytes, and a multinuclear osteoclast (black arrow) remodeling a metaphyseal trabecula.</p>
Full article ">Figure 4
<p>Histology of <span class="html-italic">R. asterias</span> pectoral fin radials. (<b>A</b>,<b>B</b>) (hematoxylin–eosin, dec. longitudinal section) High density of duplicating chondrocytes within a single lacuna and paired lacunae developing the radial (cylindrical) cartilage anlage. The matrix stained more intensely with hematoxylin corresponds to the zones of impendent mineral deposition that occur along the central axis of the radialis or in correspondence with the inter-radial amphiarthroses. Black arrows indicate the tegument. (<b>C</b>,<b>D</b>) (hematoxylin–eosin, dec., transverse section) Swellings of chondrocytes with densely stained matrix reproduce the histological features of mineral deposition of <span class="html-italic">H. sapiens</span> anlagen and show the non-remodeled texture of the calcified cartilaginous skeleton of chondrocytes (left section of figures). (*) the central cartilage core of the radials.</p>
Full article ">Figure 5
<p><span class="html-italic">Raja asterias</span> mature specimen of the inter-radial joint (toluidine blue, not declined/embedded in resin, longitudinal section). The joint consists of a layer of connective tissue (#) lying between the two discs (*) of calcified cartilage held by the branches of the central columns of the radialis. In the non-calcified cartilage matrix (weakly stained with toluidine), the tendency of the chondrocytes to align themselves into columns can be seen (arrows).</p>
Full article ">Figure 6
<p>Radiograph/morphometry of the central sector of the pectoral fin in dorso-ventral projection of an adult specimen of <span class="html-italic">R. asterias</span>. (<b>A</b>) The medial and lateral sectors are distinguished by the radials, whose two columns (superimposed in the dorso-ventral plane) run horizontally approximately halfway along the length of the fin. This diagram, reproduced from [<a href="#B6-animals-14-02575" class="html-bibr">6</a>], illustrates the irregular basal row of radial joints in the pterygium, highlighting some columns that are fused to the pterygium (*). The diagonally scaled rows of homologous radials (red line) reflect the curved profile of the entire fin margin and the gradual reduction in the number of radials in the anterior and posterior part of the fin. The symbol (^) indicates the centers of rotation of the two-column radials. (<b>B</b>) Graph showing the length (mean ± standard deviation) of the rows of radials 1–8 of the medial fin sector and 10–16 in the lateral sector; row 9 is the reference plane of the column turn in the horizontal plane. The dotted vertical line corresponds to the point of the radial sequence at which the two columns within the radial rotate in the horizontal plane.</p>
Full article ">Figure 7
<p>Transillumination and rotational dynamics of dorso-ventral columnar structures in <span class="html-italic">R. asterias</span>. Transillumination in dorso-ventral projection of the row plane, in which the dorso-ventral, superimposed columns rotate in the horizontal plane. The paired columns are held in the dorso-ventral position by the medial and lateral single discs (large arrowhead), while the lateral disc cleavage (small arrowheads) allows the columns to rotate within the visco-elastic muff of the non-calcified cartilage.</p>
Full article ">Figure 8
<p>Growth and mineral deposition in <span class="html-italic">R. asterias</span> pectoral fin radial, age group C. (<b>A</b>) Transilluminated, undecalcified specimen of the apical line of the pectoral fin rays. Mineral deposits in the form of small dark particles surround the aligned tesserae of the central column and the plates at the ends. The profile of the non-calcified cartilage cylinder is marked by red arrowheads, while the distalmost radial is still completely uncalcified. The apical fin consists of a bundle of keratin fibers between the dorsal and ventral tegument (blue arrow). (<b>B</b>) Transilluminated, undecalcified specimen of a radial in an advanced stage of calcification. The mineral deposits are compacted and form the aligned tiles of the central column with a tendency to fuse inwards. (<b>C</b>) Phase contrast image of B, confirming the pattern of the radial calcification process. (<b>D</b>) Transmitted light image, undecalcified specimen of the tiles at higher magnification. The mineral is deposited in the matrix around chondrocytes that are larger than those in the neighboring non-calcified matrix. (<b>E</b>) Phase contrast image of (<b>D</b>), showing the large chondrocytes embedded in the mineralized matrix.</p>
Full article ">Figure 9
<p>Heat-deproteinated radials of <span class="html-italic">R. asterias</span> pectoral fins of age group D (specimens 13 and 15). (<b>A</b>) Compacted mineral deposits outline the chained pattern of radial tiles in the center, but their shape is still irregular, as are the platelets at the ends. (<b>B</b>) More advanced mineralization with a regular, cylindrical shape of the tiles and plates. Regular distribution of lacunae in the calcified matrix of the plates. The dark bands separating the tiles correspond to carbon deposits of non-calcified cartilage burnt by heat treatment.</p>
Full article ">Figure 10
<p>Growth and ossification pattern of dolphin (<span class="html-italic">Tursipius truncatus</span>) fins (image reproduced from [<a href="#B7-animals-14-02575" class="html-bibr">7</a>]. (<b>A</b>) The stylopodium (1) and the two zeugopodium elements, radius (2) and ulna (3), show the ossified diaphyseal centers with flat epiphyseal ossification centers. The carpal bones, the metacarpals and the distal phalanges each have a single ossification center. White arrows indicate the distal metaphyseal growth plate cartilage of the humerus (1) and the proximal metaphyseal growth plate cartilage of the ulna (3). (<b>B</b>) The distal epiphyseal center has also developed in the radius and ulna, the proximal and distal epiphyseal centers in two metacarpals and only the proximal epiphyseal center in the first phalanges. The transverse radio-transparent lines between the diaphyseal and epiphyseal ossification centers correspond to the metaphyseal growth plate cartilage (as in terrestrial mammals) and regulate the longitudinal growth of the skeletal segment. White arrows indicate the distal metaphyseal cartilages of the radius (2) and ulna (3), as well as the proximal and distal cartilages of the 1st metacarpal. (<b>C</b>) Early fusion of the diaphyseal and epiphyseal ossification centers due to a halt in chondrocyte proliferation in the clefts of the metaphyseal growth plate. (<b>D</b>) Completed growth of the skeleton. The complete fusion of the metaphyseal cartilages indicates arrest of longitudinal growth. Comparison of the lateral and longitudinal diameter of metacarpals and phalanges indicates that the contribution of the metaphyseal plates of marine mammals to the longitudinal growth of the segment is smaller than in terrestrial mammals.</p>
Full article ">
16 pages, 6015 KiB  
Review
Coronary Artery Aneurysm or Ectasia as a Form of Coronary Artery Remodeling: Etiology, Pathogenesis, Diagnostics, Complications, and Treatment
by Patrycja Woźniak, Sylwia Iwańczyk, Maciej Błaszyk, Konrad Stępień, Maciej Lesiak, Tatiana Mularek-Kubzdela and Aleksander Araszkiewicz
Biomedicines 2024, 12(9), 1984; https://doi.org/10.3390/biomedicines12091984 - 2 Sep 2024
Viewed by 403
Abstract
Coronary artery aneurysm or ectasia (CAAE) is a term that includes both coronary artery ectasia (CAE) and coronary artery aneurysm (CAA), despite distinct phenotypes and definitions. This anomaly can be found in 0.15–5.3% of coronary angiography. CAE is a diffuse dilatation of the [...] Read more.
Coronary artery aneurysm or ectasia (CAAE) is a term that includes both coronary artery ectasia (CAE) and coronary artery aneurysm (CAA), despite distinct phenotypes and definitions. This anomaly can be found in 0.15–5.3% of coronary angiography. CAE is a diffuse dilatation of the coronary artery at least 1.5 times wider than the diameter of the normal coronary artery in a patient with a length of over 20 mm or greater than one-third of the vessel. CAE can be further subdivided into diffuse and focal dilations by the number and the length of the dilated vessels. Histologically, it presents with extensive destruction of musculoelastic elements, marked degradation of collagen and elastic fibers, and disruption of the elastic lamina. Conversely, CAA is a focal lesion manifesting as focal dilatation, which can be fusiform (if the longitudinal diameter is greater than the transverse) or saccular (if the longitudinal diameter is smaller than the transverse). Giant CAA is defined as a 4-fold enlargement of the vessel diameter and is observed in only 0.02% of patients after coronary. An aneurysmal lesion can be either single or multiple. It can be either a congenital or acquired phenomenon. The pathophysiological mechanisms responsible for the formation of CAAE are not well understood. Atherosclerosis is the most common etiology of CAAE in adults, while Kawasaki disease is the most common in children. Other etiological factors include systemic connective tissue diseases, infectious diseases, vasculitis, congenital anomalies, genetic factors, and idiopathic CAA. Invasive assessment of CAAE is based on coronary angiography. Coronary computed tomography (CT) is a noninvasive method that enables accurate evaluation of aneurysm size and location. The most common complications are coronary spasm, local thrombosis, distal embolization, coronary artery rupture, and compression of adjacent structures by giant coronary aneurysms. The approach to each patient with CAAE should depend on the severity of symptoms, anatomical structure, size, and location of the aneurysm. Treatment methods should be carefully considered to avoid possible complications of CAAE. Simultaneously, we should not unnecessarily expose the patient to the risk of intervention or surgical treatment. Patients can be offered conservative or invasive treatment. However, there are still numerous controversies and ambiguities regarding the etiology, prognosis, and treatment of patients with coronary artery aneurysms. This study summarizes the current knowledge about this disease’s etiology, pathogenesis, and management. Full article
Show Figures

Figure 1

Figure 1
<p>Possible morphologies and clinical manifestations of aneurysmal dilatation of coronary arteries. White arrow indicates the blood flow.</p>
Full article ">Figure 2
<p>Coronary angiograms showing (<b>A</b>) saccular aneurysm of the right coronary artery (arrow), (<b>B</b>) saccular aneurysm of the mid-segment of the left anterior descending artery (arrow), (<b>C</b>) fusiform aneurysm of the left anterior descending artery (arrow), (<b>D</b>) saccular aneurysm of the left main coronary artery (arrow), (<b>E</b>) coronary artery ectasia of the right coronary artery, and (<b>F</b>) coronary artery ectasia of the left circumflex artery.</p>
Full article ">Figure 3
<p>Coronary angiography of the saccular aneurysm (arrow) in the mid-segment of the left anterior descending artery.</p>
Full article ">Figure 4
<p>IVUS of the left anterior descending artery before the aneurysmal lesion, within and after the aneurysmal lesion. We have given many cross-sections to present the proximal and distal vessel references and aneurysm-to-reference ratio, showing how large the lesion is. We have also provided the legend to make it easily readable: A—aneurysm; P—proximal; D—distal; arrows—maximal vessel diameter of aneurysm.</p>
Full article ">Figure 5
<p>Coronary angiography of the fusiform aneurysm (arrow) of the left anterior descending artery.</p>
Full article ">Figure 6
<p>OCT of the left anterior descending artery before the aneurysmal lesion, within and after the aneurysmal lesion. We have given many cross-sections to present the proximal and distal vessel references and aneurysm-to-reference ratio, showing how large the lesion is. We have also provided the legend to make it easily readable: A—aneurysm; P—proximal; D—distal; arrows—maximal vessel diameter of aneurysm; asterisk—side branch.</p>
Full article ">Figure 7
<p>The aneurysmal lesion (arrow) of the left main coronary artery in CT.</p>
Full article ">Figure 8
<p>Illustration of the clinical manifestations of CAAE.</p>
Full article ">
10 pages, 4838 KiB  
Article
The Effect of Lens Focal Length on the Output Characteristics of 1.55 μm Tunable External-Cavity Semiconductor Lasers
by Xuan Li, Linyu Zhang, Wei Luo, Junce Shi, Zhaoxuan Zheng, Huiyin Kong, Meiye Qiu, Kangxun Sun, Zaijin Li, Yi Qu, Zhongliang Qiao and Lin Li
Photonics 2024, 11(9), 809; https://doi.org/10.3390/photonics11090809 - 29 Aug 2024
Viewed by 387
Abstract
The 1.55 μm TECSL has excellent characteristics such as wide tuning, narrow linewidth, high SMSR, and high output power and has a wide range of applications in optical communications, spectral sensing, gas detection, atomic physics, and biomedicine. For the TECSL, the choice of [...] Read more.
The 1.55 μm TECSL has excellent characteristics such as wide tuning, narrow linewidth, high SMSR, and high output power and has a wide range of applications in optical communications, spectral sensing, gas detection, atomic physics, and biomedicine. For the TECSL, the choice of collimating lens is very significant. In order to obtain a wider tuning range, five structures are constructed in this paper to investigate the effect of lens focal length on the output characteristics of 1.55 μm TECSL. It is shown that when the lens focal length is 4.51 mm, the minimum threshold current is 52 mA, the maximum output power is 42.36 mW, the maximum SMSR is 62.15 dB, the narrowest linewidth is 0.26 nm, and 152.3 nm (1458.2~1610.5 nm) can be tuned continuously. It is shown that different lens focal lengths affect the output characteristics of the TECSL, and the performance of the TECSL can be improved by appropriately changing the lens focal length. Full article
Show Figures

Figure 1

Figure 1
<p>Basic structure of TECSL.</p>
Full article ">Figure 2
<p>TECSL Tuning Principle.</p>
Full article ">Figure 3
<p>TECSL experimental setup.</p>
Full article ">Figure 4
<p>The 1.55 μm TECSL before and after resonance comparison. (<b>a</b>) Cavity surface spot without resonance. (<b>b</b>) Cavity surface spot with resonance.</p>
Full article ">Figure 5
<p>Tuning range of TECSL with different lens focal lengths. (<b>a</b>) Tuning range of TECSL with lens focal length of 4.51 mm. (<b>b</b>) Tuning range of TECSL with lens focal length of 2.97 mm. (<b>c</b>) Tuning range of TECSL with lens focal length of 3.10 mm. (<b>d</b>) Tuning range of TECSL with lens focal length of 5.50 mm. (<b>e</b>) Tuning range of TECSL with lens focal length of 6.20 mm.</p>
Full article ">Figure 6
<p>Threshold currents of TECSL with different lens focal lengths.</p>
Full article ">Figure 7
<p>Output power of TECSL with different lens focal lengths.</p>
Full article ">Figure 8
<p>SMSR of TECSL with different lens focal lengths.</p>
Full article ">Figure 9
<p>Maximum SMSR for TECSL with optimal focal length.</p>
Full article ">
13 pages, 2507 KiB  
Article
Controllable Preparation of Fused Silica Micro Lens Array through Femtosecond Laser Penetration-Induced Modification Assisted Wet Etching
by Kaijie Cheng, Ji Wang, Guolong Wang, Kun Yang and Wenwu Zhang
Materials 2024, 17(17), 4231; https://doi.org/10.3390/ma17174231 - 27 Aug 2024
Viewed by 314
Abstract
As an integrable micro-optical device, micro lens arrays (MLAs) have significant applications in modern optical imaging, new energy technology, and advanced displays. In order to reduce the impact of laser modification on wet etching, we propose a technique of femtosecond laser penetration-induced modification-assisted [...] Read more.
As an integrable micro-optical device, micro lens arrays (MLAs) have significant applications in modern optical imaging, new energy technology, and advanced displays. In order to reduce the impact of laser modification on wet etching, we propose a technique of femtosecond laser penetration-induced modification-assisted wet etching (FLIPM-WE), which avoids the influence of previous modification layers on subsequent laser pulses and effectively improves the controllability of lens array preparation. We conducted a detailed study on the effects of the laser single pulse energy, pulse number, and hydrofluoric acid etching duration on the morphology of micro lenses and obtained the optimal process parameters. Ultimately, two types of fused silica micro lens arrays with different focal lengths but the same numerical aperture (NA = 0.458) were fabricated using the FLPIM-WE technology. Both arrays exhibited excellent geometric consistency and surface quality (Ra~30 nm). Moreover, they achieved clear imaging at various magnifications with an adjustment range of 1.3×~3.0×. This provides potential technical support for special micro-optical systems. Full article
(This article belongs to the Special Issue Cutting Processes for Materials in Manufacturing)
Show Figures

Figure 1

Figure 1
<p>Experimental setup and method. (<b>a</b>) Steps in the fabrication of micro lens array. Step 1: using femtosecond laser-induced modification, step 2: place the modified sample in HF acid solution for ultrasonic-assisted wet etching, step 3: surface cleaning of MLA, the illustration pointed to by the black arrow shows a vertical-sectional schematic of the morphology of the microlens array; (<b>b</b>) schematic diagram of device femtosecond laser-induced modification of fused silica; (<b>c</b>) comparison between penetration FLPIM method and traditional top-down modification method.</p>
Full article ">Figure 2
<p>Influence of laser parameters on micro modified hole dimensions. (<b>a</b>) Variation in the depth of the modified holes; (<b>b</b>) variation in major axis length of the modified holes; (<b>c</b>) variation in minor axis length of the modified holes; (<b>d</b>) variation in depth-to-diameter ratio of the modified holes.</p>
Full article ">Figure 3
<p>Morphological changes of micro lens under different HF solution etching times. (<b>a</b>) 0 min; (<b>b</b>) 60 min; (<b>c</b>) 120 min; (<b>d</b>) 150 min, scale bar in <a href="#materials-17-04231-f003" class="html-fig">Figure 3</a>a,b is 10 μm; (<b>e</b>) variation in micro lens contour profiles with the etching time.</p>
Full article ">Figure 4
<p>Controlled fabrication of micro lens profiles. (<b>a</b>) Profile curves of micro lens fabricated under different pulse numbers; (<b>b</b>) depth and diameter of the micro lens fabricated under different pulse numbers. The black arrow represents the depth curve of the left coordinate axis, and the red arrow represents the diameter curve of the right coordinate axis; (<b>c</b>–<b>g</b>) three-dimensional profiles of micro lens fabricated under different pulse numbers: (<b>c</b>) 20 pulses; (<b>d</b>) 40 pulses; (<b>e</b>) 60 pulses; (<b>f</b>) 80 pulses; (<b>g</b>) 100 pulses.</p>
Full article ">Figure 5
<p>MLA schematics. (<b>a</b>) Micro lens array fabricated with a single pulse energy of 1.39 μJ and 60 pulses, scale bar: 20 μm; (<b>b</b>) micro lens array fabricated with a single pulse energy of 1.89 μJ and 80 pulses, scale bar: 20 μm; (<b>c</b>) profiles of the two micro lens arrays. The red curve represents the profile measurement result of the micro lenses within the red box in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>a. The gray curve represents the profiles measurement result of the micro lenses within the gray box in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>b; (<b>d</b>,<b>e</b>) three-dimensional views of individual micro lens structures from the two micro lens arrays.</p>
Full article ">Figure 6
<p>Imaging performance testing of the two MLAs shown in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>a,b. (<b>a</b>) Optical path diagram of the imaging analysis system. The system is equipped with optional imaging objectives; (<b>b</b>,<b>c</b>) place the MLA shown in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>a,b in the imaging analysis system, respectively. The CCD imaging results without the mask using an imaging objective of 20×. The scales are 20 μm; (<b>d1</b>–<b>d3</b>) CCD imaging results of the MLA shown in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>a after inserting the mask N. The objective lenses used are 20×, 20×, and 50× in sequence. Among them, <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>d3</b>) is the imaging pattern obtained by moving the mask upwards based on <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>d2</b>). (<b>e1</b>–<b>e3</b>) CCD imaging results under the MLA shown in <a href="#materials-17-04231-f005" class="html-fig">Figure 5</a>b using the same testing method, corresponding to <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>d1</b>)–(<b>d3</b>). The scales in <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>d1</b>,<b>e1</b>) are 20 μm. The scales in <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>d2</b>,<b>d3</b>) and <a href="#materials-17-04231-f006" class="html-fig">Figure 6</a>(<b>e2</b>,<b>e3</b>) are 20 μm.</p>
Full article ">
20 pages, 4137 KiB  
Article
A Minimal Solution Estimating the Position of Cameras with Unknown Focal Length with IMU Assistance
by Kang Yan, Zhenbao Yu, Chengfang Song, Hongping Zhang and Dezhong Chen
Drones 2024, 8(9), 423; https://doi.org/10.3390/drones8090423 - 24 Aug 2024
Viewed by 401
Abstract
Drones are typically built with integrated cameras and inertial measurement units (IMUs). It is crucial to achieve drone attitude control through relative pose estimation using cameras. IMU drift can be ignored over short periods. Based on this premise, in this paper, four methods [...] Read more.
Drones are typically built with integrated cameras and inertial measurement units (IMUs). It is crucial to achieve drone attitude control through relative pose estimation using cameras. IMU drift can be ignored over short periods. Based on this premise, in this paper, four methods are proposed for estimating relative pose and focal length across various application scenarios: for scenarios where the camera’s focal length varies between adjacent moments and is unknown, the relative pose and focal length can be computed from four-point correspondences; for planar motion scenarios where the camera’s focal length varies between adjacent moments and is unknown, the relative pose and focal length can be determined from three-point correspondences; for instances of planar motion where the camera’s focal length is equal between adjacent moments and is unknown, the relative pose and focal length can be calculated from two-point correspondences; finally, for scenarios where multiple cameras are employed for image acquisition but only one is calibrated, a method proposed for estimating the pose and focal length of uncalibrated cameras can be used. The numerical stability and performance of these methods are compared and analyzed under various noise conditions using simulated datasets. We also assessed the performance of these methods on real datasets captured by a drone in various scenes. The experimental results demonstrate that the method proposed in this paper achieves superior accuracy and stability to classical methods. Full article
Show Figures

Figure 1

Figure 1
<p><span class="html-italic">O</span><sub>1</sub> and <span class="html-italic">O</span><sub>2</sub> represent the camera center; <span class="html-italic">P</span> denotes the target feature point; <span class="html-italic">p</span><sub>1</sub> and <span class="html-italic">p</span><sub>2</sub> are the pixel coordinates of the feature points; <span class="html-italic">e</span><sub>1</sub> and <span class="html-italic">e</span><sub>2</sub> are epipoles, which are the points where the line connecting <span class="html-italic">O</span><sub>1</sub> and <span class="html-italic">O</span><sub>2</sub> intersects with the image plane; <span class="html-italic">O</span><sub>1</sub>, <span class="html-italic">O</span><sub>2</sub>, and <span class="html-italic">P</span> forms the epipolar plane; and <span class="html-italic">l</span><sub>1</sub> and <span class="html-italic">l</span><sub>2</sub> are the epipolar lines, which are the lines where the epipolar plane intersects with the image plane.</p>
Full article ">Figure 2
<p>Focal length error probability density for 10,000 randomly generated problem instances.</p>
Full article ">Figure 3
<p>Translation matrix error probability density for 10,000 randomly generated problem instances.</p>
Full article ">Figure 4
<p>Error variation curve of focal length <span class="html-italic">f</span> with different scale errors in pixel coordinates.</p>
Full article ">Figure 5
<p>Error variation curve of translation vector <b><span class="html-italic">t</span></b> with different scale errors in pixel coordinates.</p>
Full article ">Figure 6
<p>The error variation curves of eight methods when introducing different levels of noise into the three rotation angles with the IMU: (<b>a</b>) the median focal length error calculated after introducing pitch angle rotation errors; (<b>b</b>) the median focal length error calculated after introducing yaw angle rotation errors; (<b>c</b>) the median focal length error calculated after introducing roll angle rotation errors; (<b>d</b>) the median translation vector error calculated after introducing pitch angle rotation errors; (<b>e</b>) the median translation vector error calculated after introducing yaw angle rotation errors; (<b>f</b>) the median translation vector error calculated after introducing roll angle rotation errors.</p>
Full article ">Figure 7
<p>Images captured by the drone: (<b>a</b>) outdoor landscapes; (<b>b</b>) urban buildings; (<b>c</b>) road vehicles.</p>
Full article ">Figure 8
<p>Schematic of feature point extraction using the SIFT algorithm.</p>
Full article ">Figure 9
<p>Cumulative distribution functions of the estimated errors in camera focal length and translation vector across three scenarios: (<b>a</b>) the camera focal length error of outdoor landscapes; (<b>b</b>) the translation vector error of outdoor landscapes; (<b>c</b>) the camera focal length error of urban buildings; (<b>d</b>) the translation vector error of urban buildings; (<b>e</b>) the camera focal length error of road vehicles; (<b>f</b>) the translation vector error of road vehicles.</p>
Full article ">Figure 10
<p>Three-dimensional trajectory plot of real data.</p>
Full article ">Figure 11
<p>Two-dimensional trajectory plot of real data.</p>
Full article ">
25 pages, 19272 KiB  
Article
6DoF Object Pose and Focal Length Estimation from Single RGB Images in Uncontrolled Environments
by Mayura Manawadu and Soon-Yong Park
Sensors 2024, 24(17), 5474; https://doi.org/10.3390/s24175474 - 23 Aug 2024
Viewed by 689
Abstract
Accurate 6DoF (degrees of freedom) pose and focal length estimation are important in extended reality (XR) applications, enabling precise object alignment and projection scaling, thereby enhancing user experiences. This study focuses on improving 6DoF pose estimation using single RGB images of unknown camera [...] Read more.
Accurate 6DoF (degrees of freedom) pose and focal length estimation are important in extended reality (XR) applications, enabling precise object alignment and projection scaling, thereby enhancing user experiences. This study focuses on improving 6DoF pose estimation using single RGB images of unknown camera metadata. Estimating the 6DoF pose and focal length from an uncontrolled RGB image, obtained from the internet, is challenging because it often lacks crucial metadata. Existing methods such as FocalPose and Focalpose++ have made progress in this domain but still face challenges due to the projection scale ambiguity between the translation of an object along the z-axis (tz) and the camera’s focal length. To overcome this, we propose a two-stage strategy that decouples the projection scaling ambiguity in the estimation of z-axis translation and focal length. In the first stage, tz is set arbitrarily, and we predict all the other pose parameters and focal length relative to the fixed tz. In the second stage, we predict the true value of tz while scaling the focal length based on the tz update. The proposed two-stage method reduces projection scale ambiguity in RGB images and improves pose estimation accuracy. The iterative update rules constrained to the first stage and tailored loss functions including Huber loss in the second stage enhance the accuracy in both 6DoF pose and focal length estimation. Experimental results using benchmark datasets show significant improvements in terms of median rotation and translation errors, as well as better projection accuracy compared to the existing state-of-the-art methods. In an evaluation across the Pix3D datasets (chair, sofa, table, and bed), the proposed two-stage method improves projection accuracy by approximately 7.19%. Additionally, the incorporation of Huber loss resulted in a significant reduction in translation and focal length errors by 20.27% and 6.65%, respectively, in comparison to the Focalpose++ method. Full article
(This article belongs to the Special Issue Computer Vision and Virtual Reality: Technologies and Applications)
Show Figures

Figure 1

Figure 1
<p>Projection of an object onto the image plane of a pinhole camera using perspective projection.</p>
Full article ">Figure 2
<p>Initial position and orientation of the real-world chair and the image plane based on ground truth values.</p>
Full article ">Figure 3
<p>Change of the projection scale of the image after setting <math display="inline"><semantics> <msub> <mi>t</mi> <mi>z</mi> </msub> </semantics></math> to an arbitrary value.</p>
Full article ">Figure 4
<p>Obtaining the same projection size of the chair by re-scaling the focal length relative to the adjustment of <math display="inline"><semantics> <msub> <mi>t</mi> <mi>z</mi> </msub> </semantics></math>.</p>
Full article ">Figure 5
<p>Two-stage approach for predicting the 6DoF pose estimation and focal length from a single uncontrolled RGB image.</p>
Full article ">Figure 6
<p>Comparison of the outputs from the proposed method with Focalpose [<a href="#B13-sensors-24-05474" class="html-bibr">13</a>] and Focalpose++ [<a href="#B14-sensors-24-05474" class="html-bibr">14</a>] using Pix3D dataset. Subfigures (<b>a</b>–<b>t</b>) represents different classes of chair, sofa, bed and table of Pix3D Dataset. Metadata of these images are not available during the inference time.</p>
Full article ">Figure 7
<p>(<b>a</b>) Input single RGB image, (<b>b</b>) prediction from Focalpose [<a href="#B13-sensors-24-05474" class="html-bibr">13</a>], (<b>c</b>) prediction from the proposed work (Stage II output), (<b>d</b>) outputs by employing multiple refiner iterations to Stage II of the proposed approach. The green-colored contours represent the predicted pose during each iteration in the refiner of Stage II, and the red colored contour represent the ground truth.</p>
Full article ">Figure 8
<p>Distribution of <math display="inline"><semantics> <msub> <mi>t</mi> <mi>z</mi> </msub> </semantics></math> across different classes in Pix3D dataset.</p>
Full article ">
15 pages, 7791 KiB  
Article
Electro-Thermo-Mechanical Integrity of Electric Vehicle Battery Interconnects Using Micro-TIG Welding
by Ahmad Akmal Abd Manan, Amalina Amir, Nurliyana Mohamad Arifin and Ervina Efzan Mhd Noor
J. Manuf. Mater. Process. 2024, 8(4), 183; https://doi.org/10.3390/jmmp8040183 - 22 Aug 2024
Viewed by 511
Abstract
The fabrication of welded joints in steel sheets has become a focal point, especially in meeting the demands for interconnections within battery packs for electric vehicles (EVs). This study delves into the impact arising from the initiation arc during the micro-tungsten inert gas [...] Read more.
The fabrication of welded joints in steel sheets has become a focal point, especially in meeting the demands for interconnections within battery packs for electric vehicles (EVs). This study delves into the impact arising from the initiation arc during the micro-tungsten inert gas (TIG) welding of nickel-plated steel sheets. The investigation involved the manipulation of various current modulations and arc lengths. Notably, optimal results were achieved with a 5 mm arc length paired with a 25 A current modulation. Microstructural analysis, conducted through scanning electron microscopy (SEM), unveiled a higher penetration depth, contributing to a more extensive and shallower fusion zone at the interface between the filler metal and the base material. Tensile testing revealed impressive mechanical properties, with the ultimate tensile strength peaking at 90 N/mm2, a yield strength of 85 N/mm2, and the highest elastic modulus. This underscores the weld’s robustness in withstanding applied loads and resisting fracture. Furthermore, the calculation of the lowest K factor at 1.0375 indicated a reduction in resistance across the specimen, resulting in enhanced conductivity. Micro-TIG welding emerges as an efficient method for nickel-plated steel in connecting individual battery cells to form a high-capacity battery pack. These interconnections ensure efficient current flow and maintain the overall integrity and performance of the battery pack. The reliability and quality of these interconnects directly affect the battery’s efficiency, safety, and lifespan in EVs application. Full article
Show Figures

Figure 1

Figure 1
<p>Two nickel-plated steel strips and the marked welding spot.</p>
Full article ">Figure 2
<p>(<b>a</b>) The jig utilized to ensure the test sample is constrained during the welding process and (<b>b</b>) the welded test sample.</p>
Full article ">Figure 3
<p>The weld cross-section that is observed using SEM via the IMAPS program on a computer.</p>
Full article ">Figure 4
<p>(<b>a</b>) The SEM utilized to observe the molded test samples and (<b>b</b>) a simulated image to show the orientation of the molded test sample being put under the SEM.</p>
Full article ">Figure 5
<p>The designated sites for measuring the resistance of the spot weld.</p>
Full article ">Figure 6
<p>Cross-section of joint microstructures for welded nickel-plated steel sheet.</p>
Full article ">Figure 7
<p>Penetration depth and interface width for 15 A current modulation and 2 mm arc length.</p>
Full article ">Figure 8
<p>Penetration depth and interface width for 15 A current modulation and 3 mm arc length.</p>
Full article ">Figure 9
<p>The penetration depth of nickel-plated steel sheets under varying arc lengths at current modulations of (a) 15 A, (b) 20 A, and (c) 25 A.</p>
Full article ">Figure 10
<p>The interface width of nickel-plated steel sheets under varying arc lengths at current modulations of (a) 15 A, (b) 20 A, and (c) 25 A.</p>
Full article ">Figure 11
<p>The broken connections of the 5 mm arc length test sample for (<b>a</b>) 20 A and (<b>b</b>) 25 A current modulation.</p>
Full article ">Figure 12
<p>The stress–strain curve at (a) 2 mm, (b) 3 mm, (c) 4 mm, and (d) 5 mm arc length for 15 A current modulation.</p>
Full article ">Figure 13
<p>The stress–strain curve at (a) 2 mm, (b) 3 mm, (c) 4 mm, and (d) 5 mm arc length for 20 A current modulation.</p>
Full article ">Figure 14
<p>The stress–strain curve at (a) 2 mm, (b) 3 mm, (c) 4 mm, and (d) 5 mm arc length for 25 A current modulation.</p>
Full article ">Figure 15
<p>The K factor graph at different arc lengths for (a) 15 A, (b) 20 A, and (c) 25 A current modulation.</p>
Full article ">
21 pages, 12097 KiB  
Article
Infrared Camera Array System and Self-Calibration Method for Enhanced Dim Target Perception
by Yaning Zhang, Tianhao Wu, Jungang Yang and Wei An
Remote Sens. 2024, 16(16), 3075; https://doi.org/10.3390/rs16163075 - 21 Aug 2024
Viewed by 502
Abstract
Camera arrays can enhance the signal-to-noise ratio (SNR) between dim targets and backgrounds through multi-view synthesis. This is crucial for the detection of dim targets. To this end, we design and develop an infrared camera array system with a large baseline. The multi-view [...] Read more.
Camera arrays can enhance the signal-to-noise ratio (SNR) between dim targets and backgrounds through multi-view synthesis. This is crucial for the detection of dim targets. To this end, we design and develop an infrared camera array system with a large baseline. The multi-view synthesis of camera arrays relies heavily on the calibration accuracy of relative poses in the sub-cameras. However, the sub-cameras within a camera array lack strict geometric constraints. Therefore, most current calibration methods still consider the camera array as multiple pinhole cameras for calibration. Moreover, when detecting distant targets, the camera array usually needs to adjust the focal length to maintain a larger depth of field (DoF), so that the distant targets are located on the camera’s focal plane. This means that the calibration scene should be selected within this DoF range to obtain clear images. Nevertheless, the small parallax between the distant sub-aperture views limits the calibration. To address these issues, we propose a calibration model for camera arrays in distant scenes. In this model, we first extend the parallax by employing dual-array frames (i.e., recording a scene at two spatial locations). Secondly, we investigate the linear constraints between the dual-array frames, to maintain the minimum degrees of freedom of the model. We develop a real-world light field dataset called NUDT-Dual-Array using an infrared camera array to evaluate our method. Experimental results on our self-developed datasets demonstrate the effectiveness of our method. Using the calibrated model, we improve the SNR of distant dim targets, which ultimately enhances the detection and perception of dim targets. Full article
Show Figures

Figure 1

Figure 1
<p>Infrared camera array self-calibration and dim target perception framework. (<b>a</b>) Designed camera array. (<b>b</b>) Captured calibration scene. (<b>c</b>) Calibrated relative pose. (<b>d</b>) Obtained dim target. (<b>e</b>) Multi-view synthesis result.</p>
Full article ">Figure 2
<p>System outline and composition diagram.</p>
Full article ">Figure 3
<p>(<b>a</b>) Image captured by a LWIR camera. (<b>b</b>) Optical structure diagram. (<b>c</b>) LWIR camera imaging effect.</p>
Full article ">Figure 4
<p>The pipeline of our proposed method is as follows: First, dual-array frame images are obtained. Then, a correspondence search is constructed. Next, an initial image pair selection strategy across array frames is used to select the optimal image pair, and the initial two views are reconstructed. Finally, linear constraints between dual-array frames are introduced to calibrate the remaining SAIs.</p>
Full article ">Figure 5
<p>Two initial image pair adaptive selection methods. <span class="html-italic">A</span>–<span class="html-italic">I</span> are images from the left array frame, and <span class="html-italic">a</span>–<span class="html-italic">i</span> are images from the right array frame. The initial image pair selection of our strategy only needs to be considered from the across array frames.</p>
Full article ">Figure 6
<p>The linear constraint in dual-array frames. The relative poses between <span class="html-italic">A</span>–<span class="html-italic">B</span> and <span class="html-italic">a</span>–<span class="html-italic">b</span> in the dual-array frames are identical.</p>
Full article ">Figure 7
<p>A calibration result with the introduction of linear constraints in dual-array frames.</p>
Full article ">Figure 8
<p>An illustration of constant temperature heating checkerboard and the patterns in the infrared camera view.</p>
Full article ">Figure 9
<p>Mean reprojection error of infrared camera array.</p>
Full article ">Figure 10
<p>Estimated structures of four scenes. Frames from “Bike”, “Robot”, “Mind”, and “Sculpture” (<b>top</b>); structure obtained from <span class="html-italic">COLMAP</span> [<a href="#B28-remotesensing-16-03075" class="html-bibr">28</a>] (<b>second row</b>); structure obtained from <span class="html-italic">OpenSfM</span> [<a href="#B60-remotesensing-16-03075" class="html-bibr">60</a>] (<b>third row</b>); structure obtained with our method (<b>last row</b>).</p>
Full article ">Figure 11
<p>Schematic diagram of the SNR enhancement method for dim target.</p>
Full article ">Figure 12
<p>The dim target in the central sub-view (<b>top</b>); the dim target refocused in the metric calibration method [<a href="#B27-remotesensing-16-03075" class="html-bibr">27</a>] (<b>second row</b>); the dim target refocused in <span class="html-italic">OpenSfM</span> [<a href="#B60-remotesensing-16-03075" class="html-bibr">60</a>] method (<b>third row</b>); the dim target refocused in our method (<b>bottom row</b>).</p>
Full article ">Figure 13
<p>The normalized energy in the central sub-view (<b>top</b>); the normalized energy refocused in the metric calibration method [<a href="#B27-remotesensing-16-03075" class="html-bibr">27</a>] (<b>second row</b>); the normalized energy refocused in <span class="html-italic">OpenSfM</span> [<a href="#B60-remotesensing-16-03075" class="html-bibr">60</a>] method (<b>third row</b>); the normalized energy refocused in our method (<b>bottom row</b>).</p>
Full article ">
18 pages, 4494 KiB  
Article
A Novel Technique for High-Efficiency Characterization of Complex Cracks with Visual Artifacts
by Avik Kumar Das and Christopher Kin Ying Leung
Appl. Sci. 2024, 14(16), 7194; https://doi.org/10.3390/app14167194 - 15 Aug 2024
Viewed by 430
Abstract
In this paper, we introduce SHSnet, an advanced deep learning model designed for the efficient end-to-end segmentation of complex cracks, including thin, tortuous, and densely distributed ones. SHSnet features a non-uniform attention mechanism, a large receptive field, and boundary refinement to enhance segmentation [...] Read more.
In this paper, we introduce SHSnet, an advanced deep learning model designed for the efficient end-to-end segmentation of complex cracks, including thin, tortuous, and densely distributed ones. SHSnet features a non-uniform attention mechanism, a large receptive field, and boundary refinement to enhance segmentation performance while maintaining computational efficiency. To further optimize the model’s learning capability with highly imbalanced datasets, we employ a loss function (LP) based on the focal Tversky function. SHSnet shows very high performance, with values of 0.85, 0.83, 0.81, and 0.84 for precision, recall, intersection over union (IOU), and F-score, respectively. It achieves this with 10× fewer parameters than other models in the literature. Complementing SHSnet, we also present the post-processing unit (PPU), which analyzes crack morphological parameters through fracture mechanics and geometric properties. The PPU generates scanning lines to accurately compute these parameters, ensuring reliable results. The PPU shows a relative error of 0.4%, 1.2%, and 5.6% for crack number, length, and width, respectively. The methodology was benchmarked on complex ECC crack datasets as well as on multiple online datasets. In both of these cases, our results confirm that SHSnet consistently delivers superior performance and efficiency across various scenarios as compared to the methods in the literature. Full article
Show Figures

Figure 1

Figure 1
<p>Architecture of the proposed SHSnet for segmentation of thin, tortuous, and dense cracks. Here, w, h, n, and c are width, height, no. of channels, and no. of classes, respectively.</p>
Full article ">Figure 2
<p>(<b>A</b>) Receptive field (RF) for a conventional deep convolutional network. (<b>B</b>) RF for SHSnet. A wider opaque blue area represents a bigger RF.</p>
Full article ">Figure 3
<p>Effect of gamma on change in LF at different levels of accuracy.</p>
Full article ">Figure 4
<p>(<b>a</b>) Ellipse fitting on segmentation mask for crack orientation (in grey arrows). (<b>b</b>) Four scanning lines perpendicular to crack orientations.</p>
Full article ">Figure 5
<p>The development of ground truth: (<b>a</b>) original image; (<b>b</b>) rough brushing of the cracks; (<b>c</b>) color space filtering of (<b>b</b>,<b>d</b>) region; filtering of (<b>c</b>,<b>e</b>); manual improvement of (<b>d</b>).</p>
Full article ">Figure 6
<p>Effect of loss function on the segmentation results: (<b>a</b>) original photograph; (<b>b</b>) SHSnet; (<b>c</b>) SHSnet with cross-entropy (CE) loss. Note: cracks are overlaid on the original picture for better visualization. Note: the window in white is zoomed for better visualization.</p>
Full article ">Figure 7
<p>Using AI from other cementitious composites for SHCC cracks: (<b>a</b>) original photograph and results using (<b>b</b>) SHSnet, (<b>c</b>) Typical-RC-AI, and (<b>d</b>) accuracy of SHSnet at different ROIs. Note: cracks (in red) are overlaid on the original picture for better visualization.</p>
Full article ">Figure 8
<p>Evolution of crack morphological parameters with stress-strain.</p>
Full article ">Figure 9
<p>Performance of SHSnet in segmenting complex (micro)cracks on different surfaces, textures, and crack densities in the presence of visual artefacts such as loose fibers, experimental equipment, surface markings, and loose edges on images from laboratories and the literature. To summarize, in all such cases, even when the surface is unprepared and dark with high density (which even includes thin cracks propagating through surface defects as in <a href="#applsci-14-07194-f006" class="html-fig">Figure 6</a>), the segmented cracks, i.e., crack pattern, match well with manual observation. (Left: Original Image; Right: The segmentation result).</p>
Full article ">Figure 9 Cont.
<p>Performance of SHSnet in segmenting complex (micro)cracks on different surfaces, textures, and crack densities in the presence of visual artefacts such as loose fibers, experimental equipment, surface markings, and loose edges on images from laboratories and the literature. To summarize, in all such cases, even when the surface is unprepared and dark with high density (which even includes thin cracks propagating through surface defects as in <a href="#applsci-14-07194-f006" class="html-fig">Figure 6</a>), the segmented cracks, i.e., crack pattern, match well with manual observation. (Left: Original Image; Right: The segmentation result).</p>
Full article ">
9 pages, 4645 KiB  
Communication
A 2.8 W Single-Frequency Laser Output at 1064 nm from a Gradient-Doped Composite Ceramic Non-Planar Ring Oscillator
by Mingwei Gao, Yibo Ding, Qing Wang, Lei Wang, Yuan Gao, Junping Wang, Haohao Ji, Jian Zhang and Chunqing Gao
Photonics 2024, 11(8), 757; https://doi.org/10.3390/photonics11080757 - 13 Aug 2024
Viewed by 612
Abstract
An efficient Nd: A YAG single-frequency laser was demonstrated using a gradient-doped ceramic non-planar ring oscillator (NPRO). A thermal model of the gradient-doped ceramic NPRO was built to analyze the temperature field and thermal focal length. By employing a gradient-doped gain structure, the [...] Read more.
An efficient Nd: A YAG single-frequency laser was demonstrated using a gradient-doped ceramic non-planar ring oscillator (NPRO). A thermal model of the gradient-doped ceramic NPRO was built to analyze the temperature field and thermal focal length. By employing a gradient-doped gain structure, the thermal distribution within the NPRO can be effectively smoothed to reduce thermal lensing effects. Up to 2.8 W of single-frequency output power at 1064 nm from the gradient-doped ceramic NPRO was obtained, with a slope efficiency of 38%. Full article
(This article belongs to the Special Issue Narrow Linewidth Laser Sources and Their Applications)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Schematic diagram of the gradient-doped Nd: YAG ceramic; (<b>b</b>) the gradient-doped ceramic NPRO.</p>
Full article ">Figure 2
<p>Temperature distribution in NPRO with (<b>a</b>) gradient-doped composite ceramics and (<b>b</b>) 2 mm undoped end; the temperature distribution on a linear scale with (<b>c</b>) gradient-doped composite ceramics, (<b>d</b>) with 2 mm undoped end.</p>
Full article ">Figure 3
<p>Thermal focal lens versus absorbed pump power.</p>
Full article ">Figure 4
<p>Simplified layout of the laser setup used for testing the gradient-doped ceramic NPRO. L, lens; BS, beam splitter; <span class="html-italic">B</span>, magnetic field.</p>
Full article ">Figure 5
<p>Output power versus the incident pump power.</p>
Full article ">Figure 6
<p>Single-longitudinal mode operation observed with a scanning confocal Fabry–Perot (F-P) interferometer.</p>
Full article ">Figure 7
<p>Output wavelength observed with an optical spectrum analyzer.</p>
Full article ">Figure 8
<p>Heterodyne signal between a gradient-doped ceramic NPRO laser and a diffusion-bonded NPRO laser.</p>
Full article ">Figure 9
<p>Power stability of the gradient-doped ceramic NPRO laser. At 2.8 W output, the fluctuation is within 0.3% (the standard deviation of the recorded time series).</p>
Full article ">Figure 10
<p>Beam quality of the gradient-doped ceramic NPRO laser.</p>
Full article ">Figure 11
<p>Round trip loss and relaxation oscillation frequency versus the incident pump power.</p>
Full article ">
23 pages, 16139 KiB  
Article
Bioarchitectonic Nanophotonics by Replication and Systolic Miniaturization of Natural Forms
by Konstantina Papachristopoulou and Nikolaos A. Vainos
Biomimetics 2024, 9(8), 487; https://doi.org/10.3390/biomimetics9080487 - 13 Aug 2024
Viewed by 584
Abstract
The mimesis of biological mechanisms by artificial devices constitutes the modern, rapidly expanding, multidisciplinary biomimetics sector. In the broader bioinspiration perspective, however, bioarchitectures may perform independent functions without necessarily mimicking their biological generators. In this paper, we explore such Bioarchitectonic notions and demonstrate [...] Read more.
The mimesis of biological mechanisms by artificial devices constitutes the modern, rapidly expanding, multidisciplinary biomimetics sector. In the broader bioinspiration perspective, however, bioarchitectures may perform independent functions without necessarily mimicking their biological generators. In this paper, we explore such Bioarchitectonic notions and demonstrate three-dimensional photonics by the exact replication of insect organs using ultra-porous silica aerogels. The subsequent conformal systolic transformation yields their miniaturized affine ‘clones’ having higher mass density and refractive index. Focusing on the paradigms of ommatidia, the compound eye of the hornet Vespa crabro flavofasciata and the microtrichia of the scarab Protaetia cuprea phoebe, we fabricate their aerogel replicas and derivative clones and investigate their photonic functionalities. Ultralight aerogel microlens arrays are proven to be functional photonic devices having a focal length f ~ 1000 μm and f-number f/30 in the visible spectrum. Stepwise systolic transformation yields denser and affine functional elements, ultimately fused silica clones, exhibiting strong focusing properties due to their very short focal length of f ~ 35 μm and f/3.5. The fabricated transparent aerogel and xerogel replicas of microtrichia demonstrate a remarkable optical waveguiding performance, delivering light to their sub-100 nm nanotips. Dense fused silica conical clones deliver light through sub-50 nm nanotips, enabling nanoscale light–matter interactions. Super-resolution bioarchitectonics offers new and alternative tools and promises novel developments and applications in nanophotonics and other nanotechnology sectors. Full article
Show Figures

Figure 1

Figure 1
<p>SEM images of natural eyes of Vespa Crabro Flavofasciata: (<b>a</b>) Frontal view of the head. (<b>b</b>) Facets of compound eye cornea.</p>
Full article ">Figure 2
<p>SEM images of natural microtrichia of <span class="html-italic">Protaetia cuprea phoebe</span>: Microtrichia on different areas (<b>a</b>,<b>b</b>) of dorsal side of elytron. Hindwing microtrichia from two distinct areas (<b>c</b>,<b>d</b>).</p>
Full article ">Figure 3
<p>Replication of hornet’s head in aerogel: (<b>a</b>) SEM images of aerogel hornet’s head replica (far-view) and (<b>b</b>) hornet’s hexagonal microlens array structure. (<b>c</b>) microscope image of compound eye surface under the focusing condition of the schematic (<b>d</b>). (<b>e</b>) Image of focal spots under the focusing condition of the schematic (<b>f</b>).</p>
Full article ">Figure 4
<p>SEM micrographs of: (<b>a</b>) cross section of natural compound eye of hornet, where the cornea surface (A), the multilayer structure (B), and the rhabdoms (C); (<b>b</b>) close-up view and dimension bars, (<b>c</b>) aerogel replica of the compound eye at high inclination.</p>
Full article ">Figure 5
<p>Surface (full circle) and foci images (dotted circle) formed by the thick aerogel compound eye replica using blue (470 nm) and red (630 nm) filtered light. (<b>a</b>) Schematic raytracing from the second principal plane H<sub>2</sub> to the focal points for the blue F<sub>B</sub> and red F<sub>R</sub>. The back focal lengths f<sub>b</sub>(B) and f<sub>b</sub>(R) are also indicated. Image of the surface (<b>b</b>) at blue filtered light and the respective foci (<b>c</b>) are shown. Image of surface (<b>d</b>) and foci (<b>e</b>) using red filtered light. Microlens ensembles and the corresponding foci are indicated encircled.</p>
Full article ">Figure 6
<p>Xerogel replica of hornet’s head: (<b>a</b>) SEM images replica (far-view) and (<b>b</b>) close-up view of hexagonal microlens array structure. (<b>c</b>) microscope image of replica’s surface and (<b>d</b>) Image of the focal spots. Microlens ensembles and the corresponding foci in (<b>c</b>,<b>d</b>) are encircled.</p>
Full article ">Figure 7
<p>Surface (full circle) and foci images (dotted circle) formed by the thick xerogel microlens element using blue (470 nm) and red (630 nm) filtered light. Surface image (<b>a</b>) and foci image (<b>b</b>) using blue filtered light. Surface image (<b>c</b>) and foci image (<b>d</b>) using red filtered light. Microlens ensembles and the corresponding foci are indicated encircled.</p>
Full article ">Figure 8
<p>Vitrified hornet’s head replica: (<b>a</b>) SEM images replica (far-view) and (<b>b</b>) close-up view of hexagonal microlens array structure. (<b>c</b>) Microscope image of replica’s surface and (<b>d</b>) image of the respective focal spots, by use of the beam profiler. Corresponding areas of microlenses and respective foci in (<b>c</b>,<b>d</b>) are indicated encircled. (<b>e</b>) An anatomical contoured schematic of the compound eye surface superposed on the SEM image (<b>a</b>) for illustration. The values of radii of curvature of the representative contours shown are in μm.</p>
Full article ">Figure 9
<p>Aerogel replica of elytra microtrichia of the scarab: (<b>a</b>) SEM images of aerogel microtrichia array replica (far-view) and (<b>b</b>) detail of elytra microneedle structure (close-view). (<b>c</b>) microscope image of replica’s microneedles focusing on the cone base (full circle) and (<b>d</b>) image focus at the needle apex (dotted circle). Corresponding areas of cone bases in (<b>c</b>) and nanotip emission (<b>d</b>) are indicated.</p>
Full article ">Figure 10
<p>Aerogel replica of hindwing microtrichia of the scarab: (<b>a</b>–<b>c</b>) SEM images of aerogel microtrichia array replica at three different locations of the wing. (<b>d</b>) microscope image of replica’s microneedles focusing on the cone base (full circle) and on the needle apex (dotted circle).</p>
Full article ">Figure 11
<p>Xerogel replica of elytra microtrichia: (<b>a</b>,<b>b</b>) SEM images of xerogel microtrichia array replica of two different areas of the elytron. (<b>c</b>,<b>d</b>) microscope image of replica’s microneedles focusing on the needle cone base (full circle) and at the nanotip apex (dashed circle). Corresponding areas in (<b>c</b>,<b>d</b>) are indicated.</p>
Full article ">Figure 12
<p>Xerogel replicas of hindwing microtrichia of the scarab: (<b>a</b>–<b>c</b>) SEM images of xerogel microtrichia array replica at three different areas of the wing. (<b>d</b>,<b>e</b>) microscope image of replica microneedles focusing at the cone base (full circle) and at the needle apex (dotted circle). Corresponding areas in (<b>d</b>,<b>e</b>) are indicated.</p>
Full article ">Figure 13
<p>Vitrified xerogel replica of scarab hindwing microtrichia: (<b>a</b>,<b>b</b>) SEM images of sintered microtrichia array replica at two different locations of the wing. (<b>c</b>) microscope image of vitreous nanoneedles focusing on the cone base (full circle) and at the nanotip apex (dotted circle). We note that the image focus setting in these two cases is ~3 μm apart, a distance smaller than the waviness of the surface, and thus only parts of the surface can be set at sharp image focus.</p>
Full article ">
15 pages, 9001 KiB  
Article
Novel Water Probe for High-Frequency Focused Transducer Applied to Scanning Acoustic Microscopy System: Simulation and Experimental Investigation
by Van Hiep Pham, Le Hai Tran, Jaeyeop Choi, Hoanh-Son Truong, Tan Hung Vo, Dinh Dat Vu, Sumin Park and Junghwan Oh
Sensors 2024, 24(16), 5179; https://doi.org/10.3390/s24165179 - 10 Aug 2024
Viewed by 828
Abstract
A scanning acoustic microscopy (SAM) system is a common non-destructive instrument which is used to evaluate the material quality in scientific and industrial applications. Technically, the tested sample is immersed in water during the scanning process. Therefore, a robot arm is incorporated into [...] Read more.
A scanning acoustic microscopy (SAM) system is a common non-destructive instrument which is used to evaluate the material quality in scientific and industrial applications. Technically, the tested sample is immersed in water during the scanning process. Therefore, a robot arm is incorporated into the SAM system to transfer the sample for in-line inspection, which makes the system complex and increases time consumption. The main aim of this study is to develop a novel water probe for the SAM system, that is, a waterstream. During the scanning process, water was supplied using a waterstream instead of immersing the sample in the water, which leads to a simple design of an automotive SAM system and a reduction in time consumption. In addition, using a waterstream in the SAM system can avoid contamination of the sample due to immersion in water for long-time scanning. Waterstream was designed based on the measured focal length calculation of the transducer and simulated to investigate the internal flow characteristics. To validate the simulation results, the waterstream was prototyped and applied to the TSAM-400 and W-FSAM traditional and fast SAM systems to successfully image some samples such as carbon fiber-reinforced polymers, a printed circuit board, and a 6-inch wafer. These results demonstrate the design method of the water probe applied to the SAM system. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic of the TSAM−400 system with waterstream.</p>
Full article ">Figure 2
<p>Schematic of the W−FSAM system with waterstream.</p>
Full article ">Figure 3
<p>The measured focal length of transducer inside sample.</p>
Full article ">Figure 4
<p>Water domain modeling.</p>
Full article ">Figure 5
<p>Mesh construction of (<b>a</b>) water domain, (<b>b</b>) inlet, and (<b>c</b>) outlet.</p>
Full article ">Figure 6
<p>Velocity distribution inside water domain plotted as streamlines.</p>
Full article ">Figure 7
<p>Pressure distribution inside water domain plotted as streamlines.</p>
Full article ">Figure 8
<p>The velocity and pressure distribution along the centerline between the transducer and outlet.</p>
Full article ">Figure 9
<p>Waterstream design and prototype: (<b>a</b>) 2D drawing, (<b>b</b>) 3D exploded drawing, (<b>c</b>) rendered concept, (<b>d</b>) prototype.</p>
Full article ">Figure 10
<p>Rendered image of TSAM−400 system with two waterstreams.</p>
Full article ">Figure 11
<p>(<b>a</b>) CFRP sample: C-scan images of (<b>b</b>) top surface, (<b>c</b>) underlayer, and (<b>d</b>) enlarged view of underlayer.</p>
Full article ">Figure 12
<p>(<b>a</b>) PCB sample, (<b>b</b>) top surface C-scan image, (<b>c</b>) underlayer C-scan image, and (<b>d</b>) enlarged view of soldering area.</p>
Full article ">Figure 13
<p>(<b>a</b>) The 6-inch wafer sample, (<b>b</b>) C-scan image of wafer, (<b>c</b>) enlarged view of I area, (<b>d</b>) enlarged view of II area.</p>
Full article ">
12 pages, 2082 KiB  
Article
Laser Scanning Method for Time-Resolved Measurements of Wavefront Distortion Introduced by Active Elements in High-Power Laser Amplifiers
by Alyona O. Kuptsova, Gleb V. Kuptsov, Vladimir A. Petrov, Victor V. Atuchin and Victor V. Petrov
Photonics 2024, 11(8), 748; https://doi.org/10.3390/photonics11080748 - 9 Aug 2024
Viewed by 473
Abstract
A novel method was proposed for the experimental investigation of wavefront distortion introduced to amplified radiation by pumped active elements in high-power laser amplifiers. The method is based on the simultaneous measurement of temperature distribution and the distribution of population density of the [...] Read more.
A novel method was proposed for the experimental investigation of wavefront distortion introduced to amplified radiation by pumped active elements in high-power laser amplifiers. The method is based on the simultaneous measurement of temperature distribution and the distribution of population density of the excited laser level in active elements. The underlying theory of the technique was presented; various factors affecting the accuracy of wavefront distortion determination were analyzed. The method was tested to study the wavefront distortion and the depolarization of radiation introduced by the Yb:YAG active element of a cryogenically cooled laser amplifier with high-power diode pumping. The focal length of the thermal lens was 0.40 ± 0.03 and 0.47 ± 0.05 m for the horizontal and vertical planes, respectively. The focal length of the electron lens was two orders of magnitude larger. The maximum value of losses induced by depolarization was 8.5%. Full article
(This article belongs to the Special Issue New Perspectives in Ultrafast Intense Laser Science and Technology)
Show Figures

Figure 1

Figure 1
<p>Experimental setup for scanning an active element. M<sub>1</sub>, M<sub>2</sub>, M<sub>3</sub> are flat mirrors; L<sub>1</sub>, L<sub>2</sub> are focusing lenses; PBS stands for polarizing beamsplitter; photodetectors I, II are large-aperture photodiode-based detectors.</p>
Full article ">Figure 2
<p>Dynamics of the radiation transmission coefficient.</p>
Full article ">Figure 3
<p>Dependence of absorption coefficient on temperature, as measured in Yb:YAG (doping level 9.8 at.%).</p>
Full article ">Figure 4
<p>Dependence of the temperature determination error on the number of transmittance measurements.</p>
Full article ">Figure 5
<p>Contributions to the OPD profile: (<b>A</b>) thermal (radial polarization), (<b>B</b>) electronic, OPD profiles in the horizontal cross-section (<b>C</b>) for thermal contribution and (<b>D</b>) for electronic contribution.</p>
Full article ">Figure 6
<p>The fraction of depolarized radiation: (<b>A</b>) calculated from the difference in OPD for radial and tangential polarizations; (<b>B</b>) measured experimentally.</p>
Full article ">
Back to TopTop