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15 pages, 1882 KiB  
Article
Viscosity Modeling for Blood and Blood Analog Fluids in Narrow Gap and High Reynolds Numbers Flows
by Finn Knüppel, Sasha Malchow, Ang Sun, Jeanette Hussong, Alexander Hartmann, Frank-Hendrik Wurm and Benjamin Torner
Micromachines 2024, 15(6), 793; https://doi.org/10.3390/mi15060793 (registering DOI) - 16 Jun 2024
Viewed by 98
Abstract
For the optimization of ventricular assist devices (VADs), flow simulations are crucial. Typically, these simulations assume single-phase flow to represent blood flow. However, blood consists of plasma and blood cells, making it a multiphase flow. Cell migration in such flows leads to a [...] Read more.
For the optimization of ventricular assist devices (VADs), flow simulations are crucial. Typically, these simulations assume single-phase flow to represent blood flow. However, blood consists of plasma and blood cells, making it a multiphase flow. Cell migration in such flows leads to a heterogeneous cell distribution, significantly impacting flow dynamics, especially in narrow gaps of less than 300 μm found in VADs. In these areas, cells migrate away from the walls, forming a cell-free layer, a phenomenon not usually considered in current VAD simulations. This paper addresses this gap by introducing a viscosity model that accounts for cell migration in microchannels under VAD-relevant conditions. The model is based on local particle distributions measured in a microchannels with a blood analog fluid. We developed a local viscosity distribution for flows with particles/cells and a cell-free layer, applicable to both blood and analog fluids, with particle volume fractions of up to 5%, gap heights of 150 μm, and Reynolds numbers around 100. The model was validated by comparing simulation results with experimental data of blood and blood analog fluid flow on wall shear stresses and pressure losses, showing strong agreement. This model improves the accuracy of simulations by considering local viscosity changes rather than assuming a single-phase fluid. Future developments will extend the model to physiological volume fractions up to 40%. Full article
(This article belongs to the Special Issue Blood Flow in Microfluidic Medical Devices)
8 pages, 4038 KiB  
Communication
PLC-Based Polymer/Silica Hybrid Inverted Ridge LP11 Mode Rotator
by Jiaqi Liang, Daming Zhang, Xinyu Lv, Guoyan Zeng, Pai Cheng, Yuexin Yin, Xiaoqiang Sun and Fei Wang
Micromachines 2024, 15(6), 792; https://doi.org/10.3390/mi15060792 (registering DOI) - 16 Jun 2024
Viewed by 198
Abstract
The mode rotator is an important component in a PLC-based mode-division multiplexing (MDM) system, which is used to implement high-order modes with vertical intensity peaks, such as LP11b mode conversions from LP11a in PLC chips. In this paper, an LP11 [...] Read more.
The mode rotator is an important component in a PLC-based mode-division multiplexing (MDM) system, which is used to implement high-order modes with vertical intensity peaks, such as LP11b mode conversions from LP11a in PLC chips. In this paper, an LP11 mode rotator based on a polymer/silica hybrid inverted ridge waveguide is demonstrated. The proposed mode rotator is composed of an asymmetrical waveguide with a trench. According to the simulation results, the broadband conversion efficiency between the LP11a and LP11b modes is greater than 98.5%, covering the C-band after optimization. The highest mode conversion efficiency (MCE) is 99.2% at 1550 nm. The large fabrication tolerance of the proposed rotator enables its wide application in on-chip MDM systems. Full article
(This article belongs to the Section E:Engineering and Technology)
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<p>Three-dimensional (3D) schematic of the mode rotator.</p>
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<p>(<b>a</b>) Relationships between effective refractive indices of different modes with widths of core waveguides at 1550 nm while keeping <span class="html-italic">H</span> = <span class="html-italic">W</span>; optical mode distributions for the mode rotator (<b>b</b>) LP<sub>11a</sub>(E<sub>21</sub>) mode; (<b>c</b>) LP<sub>11b</sub>(E<sub>12</sub>) mode; (<b>d</b>) 1st LP<sub>11</sub> mode; (<b>e</b>) 2nd LP<sub>11</sub> mode.</p>
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<p>(<b>a</b>) Trench position <span class="html-italic">s</span>; (<b>b</b>) trench depth <span class="html-italic">d</span>; and (<b>c</b>) trench width <span class="html-italic">w</span> dependence of normalized overlap integral of 1st and 2nd LP<sub>11</sub> modes shown in <a href="#micromachines-15-00792-f002" class="html-fig">Figure 2</a>c,d, with LP<sub>11a</sub> mode at a wavelength of 1550 nm.</p>
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<p>Optimization of (<b>a</b>) trench depth <span class="html-italic">d</span>; (<b>b</b>) trench position <span class="html-italic">s</span>; (<b>c</b>) trench width <span class="html-italic">w</span>; (<b>d</b>) mode rotator length <span class="html-italic">L</span>.</p>
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<p>(<b>a</b>) Simulated modal transmission based on optimized parameters of the LP<sub>11a</sub> mode when launched at 1550 nm; (<b>b</b>) simulated modal transmission based on optimized parameters of the LP<sub>11b</sub> mode when launched at 1550 nm.</p>
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<p>Conversion efficiency of the mode rotator proposed over the C-band differed with the launch of the LP<sub>11a</sub> mode.</p>
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<p>Fabrication tolerance to (<b>a</b>) trench depth <span class="html-italic">d</span> and (<b>b</b>) trench width <span class="html-italic">w</span>.</p>
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3 pages, 286 KiB  
Editorial
3D-Printed Microdevices: From Design to Applications
by Cristiane Kalinke and Rodrigo A. A. Muñoz
Micromachines 2024, 15(6), 791; https://doi.org/10.3390/mi15060791 (registering DOI) - 15 Jun 2024
Viewed by 200
Abstract
3D printing represents an emerging technology in several fields, including engineering, medicine, and chemistry. [...] Full article
(This article belongs to the Special Issue 3D-Printed Microdevices: From Design to Applications)
18 pages, 4482 KiB  
Article
Empirical and Computational Evaluation of Hemolysis in a Microfluidic Extracorporeal Membrane Oxygenator Prototype
by Nayeem Imtiaz, Matthew D. Poskus, William A. Stoddard, Thomas R. Gaborski and Steven W. Day
Micromachines 2024, 15(6), 790; https://doi.org/10.3390/mi15060790 (registering DOI) - 15 Jun 2024
Viewed by 159
Abstract
Microfluidic devices promise to overcome the limitations of conventional hemodialysis and oxygenation technologies by incorporating novel membranes with ultra-high permeability into portable devices with low blood volume. However, the characteristically small dimensions of these devices contribute to both non-physiologic shear that could damage [...] Read more.
Microfluidic devices promise to overcome the limitations of conventional hemodialysis and oxygenation technologies by incorporating novel membranes with ultra-high permeability into portable devices with low blood volume. However, the characteristically small dimensions of these devices contribute to both non-physiologic shear that could damage blood components and laminar flow that inhibits transport. While many studies have been performed to empirically and computationally study hemolysis in medical devices, such as valves and blood pumps, little is known about blood damage in microfluidic devices. In this study, four variants of a representative microfluidic membrane-based oxygenator and two controls (positive and negative) are introduced, and computational models are used to predict hemolysis. The simulations were performed in ANSYS Fluent for nine shear stress-based parameter sets for the power law hemolysis model. We found that three of the nine tested parameters overpredict (5 to 10×) hemolysis compared to empirical experiments. However, three parameter sets demonstrated higher predictive accuracy for hemolysis values in devices characterized by low shear conditions, while another three parameter sets exhibited better performance for devices operating under higher shear conditions. Empirical testing of the devices in a recirculating loop revealed levels of hemolysis significantly lower (<2 ppm) than the hemolysis ranges observed in conventional oxygenators (>10 ppm). Evaluating the model’s ability to predict hemolysis across diverse shearing conditions, both through empirical experiments and computational validation, will provide valuable insights for future micro ECMO device development by directly relating geometric and shear stress with hemolysis levels. We propose that, with an informed selection of hemolysis parameters based on the shear ranges of the test device, computational modeling can complement empirical testing in the development of novel high-flow blood-contacting microfluidic devices, allowing for a more efficient iterative design process. Furthermore, the low device-induced hemolysis measured in our study at physiologically relevant flow rates is promising for the future development of microfluidic oxygenators and dialyzers. Full article
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<p>Comparison of different types of blood-contacting medical devices; lab-on-a-Chip, microfluidic ECMO [<a href="#B44-micromachines-15-00790" class="html-bibr">44</a>,<a href="#B45-micromachines-15-00790" class="html-bibr">45</a>], conventional ECMO [<a href="#B41-micromachines-15-00790" class="html-bibr">41</a>,<a href="#B46-micromachines-15-00790" class="html-bibr">46</a>,<a href="#B47-micromachines-15-00790" class="html-bibr">47</a>], and ventricular assist device [<a href="#B48-micromachines-15-00790" class="html-bibr">48</a>] in terms of minimum dimension of blood flow path and flow rate through the channel of minimum dimension. The height and width of the circle/oval represent the minimum dimension and flow rate ranges, respectively.</p>
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<p>(<b>a</b>) Microfluidic ECMO with ultra-thin highly permeable membrane, (<b>b</b>) blood side of the ECMO with herringbone mixers.</p>
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<p>Device variants and their corresponding flow domains. Baseline: five open channels; Reduced Gap: fewer channels with the smallest height to increase shear; Reduced Port: small inlet and outlet ports; Herringbone: channels with herringbone features to enhance mixing; herringbone height is half the channel height.</p>
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<p>Fluid path of the baseline geometry with dimensions in mm.</p>
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<p>Detail from the medium-level mesh on baseline geometry.</p>
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<p>(<b>a</b>) The predicted hemolysis increased with finer mesh. (<b>b</b>) The estimated error from true value decreased as the mesh was made finer. Error calculated using Richardson extrapolation for baseline case.</p>
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<p>Flow chart of the hemolysis incorporated via UDFs. Fluent solves for fluid flow using the core algorithms (illustrated in the right column). Hemoglobin is treated as a species with a source term that allows for the generation of hemolysis from shear stresses.</p>
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<p>(<b>a</b>) Schematic diagram of the experimental setup. (<b>b</b>) Test circuit with custom syringe pump, microfluidic devices, and blood bags.</p>
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<p>(<b>a</b>) Comparison of hemolysis data for the baseline device for both PL and TH models (total 18 variants) with Giersiepen parameters (PL 1–3), Heuser/Opitz parameters (PL 4–6), and the Zhang parameters (PL 7–9); (<b>b</b>,<b>c</b>) simulation hemolysis values for the power law model variants for all four devices and controls for flow rates 100 mL min<sup>−1</sup> (<b>b</b>) and 10 mL min<sup>−1</sup> (<b>c</b>), respectively. Panel B also includes the empirical hemolysis values.</p>
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<p>(<b>a</b>) IH% Vs. No. of Passes plotted for one empirical experiment. (<b>b</b>) Overall mean of empirical data comparing IHPP for each device and controls. The solid midline represents the median IHPP and the whiskers are the lower and upper range of IHPP. Boxes containing asterisks depicts significantly different IHPP value from the positive control (<span class="html-italic">p</span> &lt; 0.005).</p>
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<p>IH% per pass for individual devices and controls: empirical vs. simulation. The whiskers are the lower and upper range of IHPP. The squares, circles, and triangles represent Giersiepen (PL 1 to 3), Heuser/Optiz (PL 4 to 6), and Zhang (PL 7 to 9) PL model variants, respectively.</p>
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29 pages, 4670 KiB  
Review
Review on Microreactors for Photo-Electrocatalysis Artificial Photosynthesis Regeneration of Coenzymes
by Haixia Liu, Rui Sun, Yujing Yang, Chuanhao Zhang, Gaozhen Zhao, Kaihuan Zhang, Lijuan Liang and Xiaowen Huang
Micromachines 2024, 15(6), 789; https://doi.org/10.3390/mi15060789 (registering DOI) - 15 Jun 2024
Viewed by 142
Abstract
In recent years, with the outbreak of the global energy crisis, renewable solar energy has become a focal point of research. However, the utilization efficiency of natural photosynthesis (NPS) is only about 1%. Inspired by NPS, artificial photosynthesis (APS) was developed and utilized [...] Read more.
In recent years, with the outbreak of the global energy crisis, renewable solar energy has become a focal point of research. However, the utilization efficiency of natural photosynthesis (NPS) is only about 1%. Inspired by NPS, artificial photosynthesis (APS) was developed and utilized in applications such as the regeneration of coenzymes. APS for coenzyme regeneration can overcome the problem of high energy consumption in comparison to electrocatalytic methods. Microreactors represent a promising technology. Compared with the conventional system, it has the advantages of a large specific surface area, the fast diffusion of small molecules, and high efficiency. Introducing microreactors can lead to more efficient, economical, and environmentally friendly coenzyme regeneration in artificial photosynthesis. This review begins with a brief introduction of APS and microreactors, and then summarizes research on traditional electrocatalytic coenzyme regeneration, as well as photocatalytic and photo-electrocatalysis coenzyme regeneration by APS, all based on microreactors, and compares them with the corresponding conventional system. Finally, it looks forward to the promising prospects of this technology. Full article
(This article belongs to the Special Issue Microreactors and Their Applications)
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<p>Application field of artificial photosynthesis.</p>
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<p>Schematic diagram of coenzyme regeneration. (<b>A</b>) Natural photosynthesis systems [<a href="#B40-micromachines-15-00789" class="html-bibr">40</a>]. (© 2023 Wiley-VCH GmbH). (<b>B</b>) Artificial photosynthesis systems [<a href="#B39-micromachines-15-00789" class="html-bibr">39</a>]. (Copyright © 2021, Jiangnan University).</p>
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<p>Materials of microreactor. (<b>A</b>) Silicon-based microreactor [<a href="#B65-micromachines-15-00789" class="html-bibr">65</a>]. (Copyright © 2022, American Chemical Society) (<b>B</b>) Glass-based microreactor [<a href="#B68-micromachines-15-00789" class="html-bibr">68</a>]. (Copyright © 2020, Science and Technology of Advanced Materials) (<b>C</b>) Ceramic-based microreactor [<a href="#B70-micromachines-15-00789" class="html-bibr">70</a>]. (Copyright © 2009 Elsevier B.V. All rights reserved). (<b>D</b>) PDMS-based microreactor [<a href="#B73-micromachines-15-00789" class="html-bibr">73</a>]. (Copyright © 2022, Royal Society of Chemistry) (<b>E</b>) PMMA-based microreactor [<a href="#B75-micromachines-15-00789" class="html-bibr">75</a>]. (Copyright © 2020, Nano Express). (<b>F</b>) Metal-based microreactor [<a href="#B79-micromachines-15-00789" class="html-bibr">79</a>]. (Copyright © 2019, Royal Society of Chemistry). (<b>G</b>) Paper-based microreactor [<a href="#B84-micromachines-15-00789" class="html-bibr">84</a>]. (Copyright © 2020, Royal Society of Chemistry). (<b>H</b>) Cloth-based microreactor [<a href="#B89-micromachines-15-00789" class="html-bibr">89</a>]. (Copyright © 2018, Royal Society of Chemistry).</p>
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<p>Preparation technology of microreactor. (<b>A</b>) Photolithography preparation steps [<a href="#B92-micromachines-15-00789" class="html-bibr">92</a>]. (© 2021 The Authors. Published by Elsevier B.V. on behalf of Institution of Chemical Engineers). (<b>B</b>) Laser-induced hydrophilization technology [<a href="#B97-micromachines-15-00789" class="html-bibr">97</a>]. (Copyright © 2021 Elsevier B.V. All rights reserved). (<b>C</b>) Preparation step of partition method [<a href="#B102-micromachines-15-00789" class="html-bibr">102</a>]. (© 2015 The Authors. Published by WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim).</p>
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<p>Application fields of microreactors. (<b>A</b>) Microfluidic flow cytometer [<a href="#B107-micromachines-15-00789" class="html-bibr">107</a>]. (Copyright © 2020, Anal. Chem). (<b>B</b>). Cancer metastasis process [<a href="#B108-micromachines-15-00789" class="html-bibr">108</a>]. (Copyright © 2021, Signal Transduct. Target. Ther).</p>
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<p>Photocatalytic coenzyme regeneration. (<b>A</b>) HRF-Au hollow nanosphere photocatalyst [<a href="#B125-micromachines-15-00789" class="html-bibr">125</a>]. (Copyright © 2022, American Chemical Society). (<b>B</b>) Dual-functional novel core–shell nano-reactor [<a href="#B127-micromachines-15-00789" class="html-bibr">127</a>]. (Copyright © 2022, Wiley-VCH GmbH) (<b>C</b>) Blade-like photocatalytic microreactor [<a href="#B129-micromachines-15-00789" class="html-bibr">129</a>]. (Copyright © 2016, The Royal Society of Chemistry). (<b>D</b>) Capillary photocatalytic microreactor [<a href="#B132-micromachines-15-00789" class="html-bibr">132</a>]. (Copyright © 2022, Catalysis Science &amp; Technology). (<b>E</b>) Inorganic photocatalyst–enzyme system for formic acid synthesis [<a href="#B133-micromachines-15-00789" class="html-bibr">133</a>]. (Copyright © 2020, American Chemical Society). (<b>F</b>) Photoreaction zone–dark reaction zone integrated microreactor [<a href="#B134-micromachines-15-00789" class="html-bibr">134</a>]. (Copyright © 2011, The Royal Society of Chemistry). (<b>G</b>) Synthesis of L-glutamic acid [<a href="#B135-micromachines-15-00789" class="html-bibr">135</a>]. (© 2022, Elsevier B.V. All rights reserved). (<b>H</b>) Photocatalytic microcapsule reactor [<a href="#B136-micromachines-15-00789" class="html-bibr">136</a>]. (Copyright © 2018, Nanomaterials).</p>
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<p>Electrocatalytic coenzyme regeneration. (<b>A</b>) Direct electrocatalytic reaction principle [<a href="#B55-micromachines-15-00789" class="html-bibr">55</a>]. (Copyright © 2020 Wiley-VCH GmbH). (<b>B</b>) Indirect electrochemical cofactor regeneration [<a href="#B140-micromachines-15-00789" class="html-bibr">140</a>]. (Copyright © 2008 WILEY-VCH Verlag GmbH &amp; Co. KGaA, Weinheim). (<b>C</b>) Stability test results [<a href="#B141-micromachines-15-00789" class="html-bibr">141</a>]. (Copyright © 2019 American Chemical Society). (<b>D</b>) UV–vis absorption spectra of products obtained before (a) and after (b) adding alcohol dehydrogenase and acetaldehyde [<a href="#B144-micromachines-15-00789" class="html-bibr">144</a>]. (Copyright © 2022, ACS Appl. Mater. Interfaces). (<b>E</b>) A schematic diagram of the influence of electrocatalytic potential on the regeneration yield of coenzyme [<a href="#B146-micromachines-15-00789" class="html-bibr">146</a>]. (© 2017 Elsevier Ltd. All rights reserved). (<b>F</b>) A schematic diagram of the influence of electric field on the regeneration yield of coenzyme [<a href="#B147-micromachines-15-00789" class="html-bibr">147</a>]. (© 2021 Wiley-VCH GmbH). (<b>G</b>) Average sensitivity and linearity of array-flexible lactic acid enzymatic biosensor [<a href="#B148-micromachines-15-00789" class="html-bibr">148</a>]. (© 2017 Elsevier Ltd. All rights reserved).</p>
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<p>Photo-electrocatalysis coenzyme regeneration. (<b>A</b>) Regeneration scheme of coenzyme in photocathode [<a href="#B150-micromachines-15-00789" class="html-bibr">150</a>]. (Copyright © 2023, J. Am. Chem. Soc.). (<b>B</b>) Schematic diagram of photocatalytic coenzyme regeneration in photocathode in presence of M [<a href="#B151-micromachines-15-00789" class="html-bibr">151</a>]. (Copyright © 2024, American Chemical Society) (<b>C</b>) Linear sweep voltammetry (LSV) scanning characterization of hematite before and after Co-Pi deposition under visible light chopping illumination. [<a href="#B152-micromachines-15-00789" class="html-bibr">152</a>]. (© 2017, Wiley-VCH Verlag GmbH &amp; Co. KGaA, Weinheim) (<b>D</b>) SEM characterization of ITO conductive glass modified by PDDS/TiO<sub>2</sub> film [<a href="#B153-micromachines-15-00789" class="html-bibr">153</a>]. (Copyright © 2011, Elsevier B.V. All rights reserved.) (<b>E</b>) LSV scanning curve of PFP-PAs under condition of no light and illumination [<a href="#B154-micromachines-15-00789" class="html-bibr">154</a>]. (© 2020, Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.) (<b>F</b>) HAADF-STEM characterization of metal–organic frameworks [<a href="#B155-micromachines-15-00789" class="html-bibr">155</a>]. (Copyright © 2022, American Chemical Society) (<b>G</b>) Physical diagram of photo-electric catalytic microreactor [<a href="#B156-micromachines-15-00789" class="html-bibr">156</a>]. (Copyright © 2012, The Royal Society of Chemistry) (<b>H</b>) Schematic diagram of continuous photo-electrocatalytic microreactor [<a href="#B157-micromachines-15-00789" class="html-bibr">157</a>]. (Copyright © 2019, The Royal Society of Chemistry) (<b>I</b>) SEM image of anodic titanium oxide coil [<a href="#B158-micromachines-15-00789" class="html-bibr">158</a>] (© 2016, The Korean Society of Industrial and Engineering Chemistry. Published by Elsevier B.V. All rights reserved).</p>
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18 pages, 4232 KiB  
Article
Design and Evaluation of an Eye Mountable AutoDALK Robot for Deep Anterior Lamellar Keratoplasty
by Justin D. Opfermann, Yaning Wang, James Kaluna, Kensei Suzuki, William Gensheimer, Axel Krieger and Jin U. Kang
Micromachines 2024, 15(6), 788; https://doi.org/10.3390/mi15060788 (registering DOI) - 15 Jun 2024
Viewed by 152
Abstract
Partial-thickness corneal transplants using a deep anterior lamellar keratoplasty (DALK) approach has demonstrated better patient outcomes than a full-thickness cornea transplant. However, despite better clinical outcomes from the DALK procedure, adoption of the technique has been limited because the accurate insertion of the [...] Read more.
Partial-thickness corneal transplants using a deep anterior lamellar keratoplasty (DALK) approach has demonstrated better patient outcomes than a full-thickness cornea transplant. However, despite better clinical outcomes from the DALK procedure, adoption of the technique has been limited because the accurate insertion of the needle into the deep stroma remains technically challenging. In this work, we present a novel hands-free eye mountable robot for automatic needle placement in the cornea, AutoDALK, that has the potential to simplify this critical step in the DALK procedure. The system integrates dual light-weight linear piezo motors, an OCT A-scan distance sensor, and a vacuum trephine-inspired design to enable the safe, consistent, and controllable insertion of a needle into the cornea for the pneumodissection of the anterior cornea from the deep posterior cornea and Descemet’s membrane. AutoDALK was designed with feedback from expert corneal surgeons and performance was evaluated by finite element analysis simulation, benchtop testing, and ex vivo experiments to demonstrate the feasibility of the system for clinical applications. The mean open-loop positional deviation was 9.39 µm, while the system repeatability and accuracy were 39.48 µm and 43.18 µm, respectively. The maximum combined thrust of the system was found to be 1.72 N, which exceeds the clinical penetration force of the cornea. In a head-to-head ex vivo comparison against an expert surgeon using a freehand approach, AutoDALK achieved more consistent needle depth, which resulted in fewer perforations of Descemet’s membrane and significantly deeper pneumodissection of the stromal tissue. The results of this study indicate that robotic needle insertion has the potential to simplify the most challenging task of the DALK procedure, enable more consistent surgical outcomes for patients, and standardize partial-thickness corneal transplants as the gold standard of care if demonstrated to be more safe and more effective than penetrating keratoplasty. Full article
(This article belongs to the Section B:Biology and Biomedicine)
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<p>Isometric (<b>a</b>) and cross-sectional view (<b>b</b>) of the AutoDALK robot mounted on an eye. The 25 G needle with the OCT fiber is shown in the dashed box. A 2 cm scale bar is shown.</p>
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<p>Prototype of the piezo-based eye mountable AutoDALK system with key features identified (<b>a</b>). A three-dimensional rendering of the front (<b>b</b>) and top view (<b>c</b>) with key dimensions labelled.</p>
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<p>Illustration of the AutoDALK setup for ex vivo testing in porcine eye (<b>a</b>), with 100× microscope image of the 25 G needle tip with embedded lensed OCT fiber (<b>b</b>). A−scans from the fiber are collected by the common path swept source OCT system illustrated in the block diagram (<b>c</b>), and then displayed to the user as a depth map where distance between the needle tip and DM at the beginning (<b>d</b>-<b>left</b>) and end (<b>d</b>-<b>right</b>) can be visualized.</p>
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<p>AutoDALK clinical workflow.</p>
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<p>Finite element analysis illustrating fixtures (green arrows) and applied forces (pink arrows) (<b>a</b>), mesh analysis (<b>b</b>), resulting stress (<b>c</b>), and deflection (<b>d</b>) with average values calculated from samples in the circled regions.</p>
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<p>Accuracy and repeatability test setup using a 25 G needle with embedded OCT.</p>
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<p>Motor thrust test setup (<b>a</b>) and the motor’s resulting maximum thrust profile for different speeds (<b>b</b>). The clinical force requirement for cornea penetration is shown with a horizontal line.</p>
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<p>Experimental results for the AutoDALK (<b>a</b>–<b>d</b>) and freehand (<b>e</b>–<b>h</b>) approaches. Representative images of the surgical approach (<b>a</b>,<b>e</b>), final needle depth with an arrow at the needle tip and a dashed line identifying the endothelial layer (<b>b</b>,<b>f</b>), pneumodissection result with the level of dissection shown by an arrow (<b>c</b>,<b>g</b>) and endothelium at the top of image, and color image of resulting stromal blanching (<b>d</b>,<b>g</b>).</p>
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<p>Representative intraoperative OCT A-scan images during ex vivo experiments showing the needle and DM at the start (<b>a</b>), middle (<b>b</b>,<b>c</b>), and end (<b>d</b>) of the procedure.</p>
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<p>Box-and-whisker plot illustrating the difference in needle depth variance between approaches.</p>
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<p>Illustrating the injection angle, θ, injection force, F, and the downward component of the injection force, F<sub>y</sub>, for a needle just prior to pneumodissection.</p>
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6 pages, 982 KiB  
Editorial
Editorial for the Special Issue on Laser Additive Manufacturing: Design, Materials, Processes, and Applications, 2nd Edition
by Jie Yin, Yang Liu, Linda Ke and Kai Guan
Micromachines 2024, 15(6), 787; https://doi.org/10.3390/mi15060787 (registering DOI) - 15 Jun 2024
Viewed by 187
Abstract
Laser-based additive manufacturing (LAM) represents one of the most forward-thinking transformations in how we conceive, design, and bring to life engineered solutions [...] Full article
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<p>Topics covered in the Special Issue titled “Laser Additive Manufacturing: Design, Materials, Processes, and Applications, 2nd Edition”.</p>
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10 pages, 5241 KiB  
Article
Harnessing Standing Sound Waves to Treat Intraocular Blood Cell Accumulation
by Avraham Kenigsberg, Shany Shperling, Ornit Nagler-Avramovitz, Heli Peleg-Levy, Silvia Piperno, Alon Skaat, Ari Leshno, Hagay Shpaisman and Noa Kapelushnik
Micromachines 2024, 15(6), 786; https://doi.org/10.3390/mi15060786 (registering DOI) - 15 Jun 2024
Viewed by 225
Abstract
Certain ocular conditions result from the non-physiological presence of intraocular particles, leading to visual impairment and potential long-term damage. This happens when the normally clear aqueous humor becomes less transparent, thus blocking the visual axis and by intraocular pressure elevation due to blockage [...] Read more.
Certain ocular conditions result from the non-physiological presence of intraocular particles, leading to visual impairment and potential long-term damage. This happens when the normally clear aqueous humor becomes less transparent, thus blocking the visual axis and by intraocular pressure elevation due to blockage of the trabecular meshwork, as seen in secondary open-angle glaucoma (SOAG). Some of these “particle-related pathologies” acquire ocular conditions like pigment dispersion syndrome, pseodoexfoliation and uveitis. Others are trauma-related, such as blood cell accumulation in hyphema. While medical and surgical treatments exist for SOAG, there is a notable absence of effective preventive measures. Consequently, the prevailing clinical approach predominantly adopts a “wait and see” strategy, wherein the focus lies on managing secondary complications and offers no treatment options for particulate matter disposal. We developed a new technique utilizing standing acoustic waves to trap and direct intraocular particles. By employing acoustic trapping at nodal regions and controlled movement of the acoustic transducer, we successfully directed these particles to specific locations within the angle. Here, we demonstrate control and movement of polystyrene (PS) particles to specific locations within an in vitro eye model, as well as blood cells in porcine eyes (ex vivo). The removal of particles from certain areas can facilitate the outflow of aqueous humor (AH) and help maintain optimal intraocular pressure (IOP) levels, resulting in a non-invasive tool for preventing secondary glaucoma. Furthermore, by controlling the location of trapped particles we can hasten the clearance of the AH and improve visual acuity and quality more effectively. This study represents a significant step towards the practical application of our technique in clinical use. Full article
(This article belongs to the Special Issue Acoustical Tweezers: From Fundamental Research to Applications)
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<p>Illustration of interocular particles trapped and directed utilizing the acoustic method presented in this manuscript. An acoustic transducer generates standing acoustic waves to guide intraocular particles toward nodal areas. Subsequent mechanical movement of the transducer induces a downward pull on the particles.</p>
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<p>(<b>a</b>) Side view of the intraocular manipulation device. (<b>b</b>) Rear view (eye side) of the 3D-printed reservoir housing the acoustic resonator. (<b>c</b>) Front view (camera side) of the 3D-printed reservoir housing the acoustic resonator. (<b>d</b>) Eye model depicting PS particles within the anterior chamber. (<b>e</b>) Front view of an eye model attached to the 3D reservoir. (<b>f</b>) Side view of an eye model attached to the 3D reservoir.</p>
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<p>(<b>a</b>) Illustration of the acoustic resonator (green outline) movement along the Z-axis during one run and of the (<b>b</b>) top view of the acoustic resonator and eye positions during a run. (<b>c</b>) AC eye model after PS injection (before the run). (<b>d</b>) AC model during the run. (<b>e</b>) AC model after the run ended.</p>
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<p>Average change in polystyrene (PS) height with gravitation only (30 min), as a reference, and with acoustic treatment (3 runs).</p>
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<p>Microscope images of a vertically positioned porcine eye with human blood. The visual axis is marked by an orange circle: (<b>a</b>) initial state. (<b>b</b>) After 21 min without acoustic waves. Minimal sinking is observed. (<b>c</b>) End of the first run. (<b>d</b>) End of the second run. (<b>e</b>) End of the third run. (<b>f</b>) Changes in blood cell height (as a percentage of the anterior chamber height) due to gravity and during treatment in a single experiment.</p>
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<p>Histology of the angle in treated and non-treated eyes. (<b>a</b>) Illustration of the AC following treatment with an acoustic wave to inferiorly displace the RBCs. (<b>a</b>,<b>b</b>) Histology sections of the upper portion of the angle showing minimal numbers of red blood cells in the treated eye (<b>b</b>), and a large number of red blood cells in the non-treated eye (<b>c</b>, yellow arrow). (<b>d</b>) High magnification of the lower angle of a treated eye showing a large number of condensed red blood cells. (<b>e</b>,<b>f</b>, yellow arrow) Histology sections of the lower angle showing a larger number of red blood cells in the treated eye (<b>e</b>) compared with the non-treated eye (<b>f</b>).</p>
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14 pages, 958 KiB  
Article
Rapid Fabrication of Tungsten Oxide-Based Electrochromic Devices through Femtosecond Laser Processing
by Liqun Wang, Zihao Zhai and Longnan Li
Micromachines 2024, 15(6), 785; https://doi.org/10.3390/mi15060785 (registering DOI) - 14 Jun 2024
Viewed by 101
Abstract
The sol-gel method is a widely adopted technique for the preparation of tungsten trioxide (WO₃) materials, favored for its cost-effectiveness and straightforward production procedures. However, this method encounters challenges such as prolonged annealing periods and limited flexibility in fabricating patterned WO₃ films. This [...] Read more.
The sol-gel method is a widely adopted technique for the preparation of tungsten trioxide (WO₃) materials, favored for its cost-effectiveness and straightforward production procedures. However, this method encounters challenges such as prolonged annealing periods and limited flexibility in fabricating patterned WO₃ films. This study introduces a novel approach that integrates femtosecond laser processing with the sol-gel method to enhance the fabrication of WO₃ films. By adjusting polyvinylpyrrolidone (PVP) concentrations during sol-gel synthesis, precise control over film thickness and optimized film properties were achieved. The innovative technique significantly reduced the annealing time required to achieve an 80% transmittance rate from 90 min to 40 min, marking a 56% decrease. Laser processing increased the surface roughness of the films from Sa = 0.032 to Sa = 0.119, facilitating enhanced volatilization of organics during heat treatment. Additionally, this method improved the transmittance modulation of the films by 22% at 550 nm compared to unprocessed counterparts. This approach not only simplifies the manufacturing process but also enhances the optical efficiency of electrochromic devices, potentially leading to broader applications and more effective energy conservation strategies. Full article
(This article belongs to the Special Issue Micro/Nanostructures in Sensors and Actuators)
20 pages, 6151 KiB  
Article
Size-Effect-Based Dimension Compensations in Wet Etching for Micromachined Quartz Crystal Microstructures
by Yide Dong, Guangbin Dou, Zibiao Wei, Shanshan Ji, Huihui Dai, Kaiqin Tang and Litao Sun
Micromachines 2024, 15(6), 784; https://doi.org/10.3390/mi15060784 - 14 Jun 2024
Viewed by 149
Abstract
Microfabrication technology with quartz crystals is gaining importance as the miniaturization of quartz MEMS devices is essential to ensure the development of portable and wearable electronics. However, until now, there have been no reports of dimension compensation for quartz device fabrication. Therefore, this [...] Read more.
Microfabrication technology with quartz crystals is gaining importance as the miniaturization of quartz MEMS devices is essential to ensure the development of portable and wearable electronics. However, until now, there have been no reports of dimension compensation for quartz device fabrication. Therefore, this paper studied the wet etching process of Z-cut quartz crystal substrates for making deep trench patterns using Au/Cr metal hard masks and proposed the first quartz fabrication dimension compensation strategy. The size effect of various sizes of hard mask patterns on the undercut developed in wet etching was experimentally investigated. Quartz wafers masked with initial vias ranging from 3 μm to 80 μm in width were etched in a buffered oxide etch solution (BOE, HF:NH4F = 3:2) at 80 °C for prolonged etching (>95 min). It was found that a larger hard mask width resulted in a smaller undercut, and a 30 μm difference in hard mask width would result in a 17.2% increase in undercut. In particular, the undercuts were mainly formed in the first 5 min of etching with a relatively high etching rate of 0.7 μm/min (max). Then, the etching rate decreased rapidly to 27%. Furthermore, based on the etching width compensation and etching position compensation, new solutions were proposed for quartz crystal device fabrication. And these two kinds of compensation solutions were used in the fabrication of an ultra-small quartz crystal tuning fork with a resonant frequency of 32.768 kHz. With these approaches, the actual etched size of critical parts of the device only deviated from the designed size by 0.7%. And the pattern position symmetry of the secondary lithography etching process was improved by 96.3% compared to the uncompensated one. It demonstrated significant potential for improving the fabrication accuracy of quartz crystal devices. Full article
(This article belongs to the Special Issue Two-Dimensional Materials for Electronic and Optoelectronic Devices)
13 pages, 1422 KiB  
Article
Influence of Anode Immersion Speed on Current and Power in Plasma Electrolytic Polishing
by Joško Valentinčič, Henning Zeidler, Toni Böttger and Marko Jerman
Micromachines 2024, 15(6), 783; https://doi.org/10.3390/mi15060783 - 14 Jun 2024
Viewed by 202
Abstract
Plasma electrolytic polishing (PeP) is mainly used to improve the surface quality and thus the performance of electrically conductive parts. It is usually used as an anodic process, i.e., the workpiece is positively charged. However, the process is susceptible to high current peaks [...] Read more.
Plasma electrolytic polishing (PeP) is mainly used to improve the surface quality and thus the performance of electrically conductive parts. It is usually used as an anodic process, i.e., the workpiece is positively charged. However, the process is susceptible to high current peaks during the formation of the vapour–gaseous envelope, especially when polishing workpieces with a large surface area. In this study, the influence of the anode immersion speed on the current peaks and the average power during the initialisation of the PeP process is investigated for an anode the size of a microreactor mould insert. Through systematic experimentation and analysis, this work provides insights into the control of the initialisation process by modulating the anode immersion speed. The results clarify the relationship between immersion speed, peak current, and average power and provide a novel approach to improve process efficiency in PeP. The highest peak current and average power occur when the electrolyte splashes over the top of the anode and not, as expected, when the anode touches the electrolyte. By immersion of the anode while the voltage is applied to the anode and counterelectrode, the reduction of both parameters is over 80%. Full article
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<p>The acquisition system to monitor the voltage and current signals during PeP.</p>
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<p>Current and voltage waveform acquired during the process initialisation with submerged anode. The power waveform is calculated in Matlab<sup>®</sup> programming environment. The initialisation process is highly power-demanding, dynamic, and repeatable.</p>
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<p>Waveforms acquired and calculated at immersion speed 5 mm · s<sup>−1</sup>. No significant current peaks are identified, and the highest power appears during splashing the electrolyte over the anode top surface.</p>
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<p>Current peaks in the contact time domain and the time of its appearance measured from the time when anode touches the electrolyte surface for various immersion speeds, when the anode position is fixed at touching the electrolyte surface, and when it is submerged.</p>
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<p>Waveforms at immersion speed 400 mm · s<sup>−1</sup> and current and power peaks indicated by red circles in contact and splashing time domain.</p>
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<p>Current peaks for all immersion speeds in contact and splashing time domain. The blue continuous horizontal line represents the average current in stable polishing and the dotted lines its standard deviation.</p>
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<p>Average power for all immersion speeds in contact and splashing time domain. The blue continuous horizontal line represents the average power in stable polishing and the dotted lines its standard deviation.</p>
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11 pages, 7680 KiB  
Article
Characterization of Magnetorheological Impact Foams in Compression
by Young Choi and Norman M. Wereley
Micromachines 2024, 15(6), 782; https://doi.org/10.3390/mi15060782 - 14 Jun 2024
Viewed by 189
Abstract
This study focuses on the development and compressive characteristics of magnetorheological elastomeric foam (MREF) as an adaptive cushioning material designed to protect payloads from a broader spectrum of impact loads. The MREF exhibits softness and flexibility under light compressive loads and low strains, [...] Read more.
This study focuses on the development and compressive characteristics of magnetorheological elastomeric foam (MREF) as an adaptive cushioning material designed to protect payloads from a broader spectrum of impact loads. The MREF exhibits softness and flexibility under light compressive loads and low strains, yet it becomes rigid in response to higher impact loads and elevated strains. The synthesis of MREF involved suspending micron-sized carbonyl Fe particles in an uncured silicone elastomeric foam. A catalyzed addition crosslinking reaction, facilitated by platinum compounds, was employed to create the rapidly setting silicone foam at room temperature, simplifying the synthesis process. Isotropic MREF samples with varying Fe particle volume fractions (0%, 2.5%, 5%, 7.5%, and 10%) were prepared to assess the effect of particle concentrations. Quasi-static and dynamic compressive stress tests on the MREF samples placed between two multipole flexible strip magnets were conducted using an Instron servo-hydraulic test machine. The tests provided measurements of magnetic field-sensitive compressive properties, including compression stress, energy absorption capability, complex modulus, and equivalent viscous damping. Furthermore, the experimental investigation also explored the influence of magnet placement directions (0° and 90°) on the compressive properties of the MREFs. Full article
(This article belongs to the Special Issue Magnetorheological Materials and Application Systems)
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<p>Square-shaped isotropic magnetorheological elastomeric foam (MREF) samples fabricated with different carbonyl Fe particle concentrations (nominal size: 50.8 mm × 50.8 mm × 12.7 mm).</p>
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<p>Magnetic density of the flexible multipole strip magnet with respect to the length and width (<math display="inline"><semantics> <msub> <mi>B</mi> <mrow> <mi>R</mi> <mi>M</mi> <mi>S</mi> </mrow> </msub> </semantics></math> = 104 mT and 8 poles per inch).</p>
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<p>Experimental setup of the compressive test of the MREF samples by using an Instron servo-hydraulic test machine.</p>
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<p>Schematic diagram for the magnetic placement directions for the MREF samples. Here, the blue and red colors mean the magnetic poles.</p>
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<p>Compressive stress versus strain curves for isotropic MREF samples with Fe particle concentrations of 0 and 10 vol%. (<b>a</b>) 0 vol% (No Fe particle); (<b>b</b>) 10 vol%.</p>
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<p>Compressive stress versus particle concentration for the MREFs for a range of discrete strain (<math display="inline"><semantics> <mi>ϵ</mi> </semantics></math>) levels. (<b>a</b>) with magnets (0<math display="inline"><semantics> <mo>°</mo> </semantics></math>); (<b>b</b>) with magnets (90<math display="inline"><semantics> <mo>°</mo> </semantics></math>).</p>
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<p>Cushioning index and energy absorption density of the MREFs versus particle concentration. (<b>a</b>) cushioning index; (<b>b</b>) energy absorption density.</p>
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<p>Complex modulus and equivalent viscous damping of the MREFs with Fe particle concentrations of 0 and 10 vol% in the frequency domain. (<b>a</b>) complex modulus; (<b>b</b>) equivalent viscous damping.</p>
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<p>Maximum complex modulus and equivalent viscous damping of the MREFs versus particle concentration. (<b>a</b>) maximum complex modulus; (<b>b</b>) maximum equivalent viscous dammping.</p>
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11 pages, 7214 KiB  
Article
Enhancing GaN/AlxGa1−xN-Based Heterojunction Phototransistors: The Role of Graded Base Structures in Performance Improvement
by Lingxia Zhang, Hualong Wu, Chenguang He, Kang Zhang, Yunzhou Liu, Qiao Wang, Longfei He, Wei Zhao and Zhitao Chen
Micromachines 2024, 15(6), 778; https://doi.org/10.3390/mi15060778 - 13 Jun 2024
Viewed by 158
Abstract
This research explores the architecture and efficacy of GaN/AlxGa1−xN-based heterojunction phototransistors (HPTs) engineered with both a compositionally graded and a doping-graded base. Employing theoretical analysis along with empirical fabrication techniques, HPTs configured with an aluminum compositionally graded base were [...] Read more.
This research explores the architecture and efficacy of GaN/AlxGa1−xN-based heterojunction phototransistors (HPTs) engineered with both a compositionally graded and a doping-graded base. Employing theoretical analysis along with empirical fabrication techniques, HPTs configured with an aluminum compositionally graded base were observed to exhibit a substantial enhancement in current gain. Specifically, theoretical models predicted a 12-fold increase, while experimental evaluations revealed an even more pronounced improvement of approximately 27.9 times compared to conventional GaN base structures. Similarly, HPTs incorporating a doping-graded base demonstrated significant gains, with theoretical predictions indicating a doubling of current gain and experimental assessments showing a 6.1-fold increase. The doping-graded base implements a strategic modulation of hole concentration, ranging from 3.8 × 1016 cm−3 at the base–emitter interface to 3.8 × 1017 cm−3 at the base–collector junction. This controlled gradation markedly contributes to the observed enhancements in current gain. The principal mechanism driving these improvements is identified as the increased electron drift within the base, propelled by the intrinsic electric field inherent to both the compositionally and doping-graded structures. These results highlight the potential of such graded base designs in enhancing the performance of GaN/AlxGa1−xN HPTs and provide crucial insights for the advancement of future phototransistor technologies. Full article
(This article belongs to the Special Issue GaN Heterostructure Devices: From Materials to Application)
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<p>A schematic of the complete GaN/Al<sub>x</sub>Ga<sub>1−x</sub>N HPT structures.</p>
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<p>AFM images (5 μm × 5 μm) of Structures (<b>a</b>) A, (<b>b</b>) B, and (<b>c</b>) C.</p>
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<p>I–V characteristics of (<b>a</b>) Structure A, (<b>b</b>) Structure B and (<b>c</b>) Structure C under dark and UV illuminations.</p>
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<p>Comparison of (<b>a</b>) dark and (<b>b</b>) illuminated current of the three structures.</p>
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14 pages, 5979 KiB  
Article
Design, Fabrication, Characterization, and Simulation of AlN-Based Piezoelectric Micromachined Ultrasonic Transducer for Sonar Imaging Applications
by Wenxing Chen, Shenglin Ma, Xiaoyi Lai, Zhizhen Wang, Hui Zhao, Qiang Zha, Yihsiang Chiu and Yufeng Jin
Micromachines 2024, 15(6), 781; https://doi.org/10.3390/mi15060781 - 13 Jun 2024
Viewed by 205
Abstract
To address the requirements of sonar imaging, such as high receiving sensitivity, a wide bandwidth, and a wide receiving angle, an AlN PMUT with an optimized ratio of 0.6 for the piezoelectric layer diameter to backside cavity diameter is proposed in this paper. [...] Read more.
To address the requirements of sonar imaging, such as high receiving sensitivity, a wide bandwidth, and a wide receiving angle, an AlN PMUT with an optimized ratio of 0.6 for the piezoelectric layer diameter to backside cavity diameter is proposed in this paper. A sample AlN PMUT is designed and fabricated with the SOI substrate-based bulk MEMS process. The characterization test result of the sample demonstrates a −6 dB bandwidth of approximately 500 kHz and a measured receiving sensitivity per unit area of 1.37 V/μPa/mm2, which significantly surpasses the performance of previously reported PMUTs. The −6 dB horizontal angles of the AlN PMUT at 300 kHz and 500 kHz are measured as 68.30° and 54.24°, respectively. To achieve an accurate prediction of its characteristics when being packaged and assembled in a receive array, numerical simulations with the consideration of film stress are conducted. The numerical result shows a maximum deviation of ±7% in the underwater receiving sensitivity across the frequency range of 200 kHz to 1000 kHz and a deviation of about 0.33% in the peak of underwater receiving sensitivity compared to the experimental data. By such good agreement, the simulation method reveals its capability of providing theoretical foundation for enhancing the uniformity of AlN PMUTs in future studies. Full article
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<p>Schematic of PMUT cross section and simulation model.</p>
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<p>Potential simulation results of PMUT with different piezoelectric dimensions, listed as follows: (<b>a</b>) R1:R2 = 1.1; (<b>b</b>) R1:R2 = 0.6.</p>
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<p>Simulation results of deflection of suspended stacked film at center with AlN piezoelectric layer under different residual stress conditions.</p>
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<p>Resonance frequency simulation results of PMUT with AlN piezoelectric layer under different residual stress conditions.</p>
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<p>The process flow of the PMUTs.</p>
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<p>SEM image of PMUT cross section.</p>
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<p>(<b>a</b>) Optical microscope image of PMUTs. (<b>b</b>) Optical microscope image of cavity.</p>
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<p>Measurements of resonant frequency of PMUTs in air.</p>
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<p>The measurement results of deflection at the center of the film.</p>
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<p>A schematic diagram of the test system for PMUT underwater receiving sensitivity.</p>
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<p>Measurement results of PMUT receiving signals at 300 kHz.</p>
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<p>(<b>a</b>) A schematic diagram of the measurement system for the receiving angle. (<b>b</b>) Measurements of the horizontal angle of the PMUTs.</p>
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<p>Simulation model of PMUT acoustic characteristics considering residual stress.</p>
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<p>PMUT acoustic receiving simulation results. (<b>a</b>) Sound pressure distribution. (<b>b</b>) Echo signals with frequencies ranging from 200 kHz to 1000 kHz.</p>
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<p>Simulation and measurement results of PMUTs’ underwater receiving sensitivity (<b>a</b>) and relative error (<b>b</b>).</p>
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13 pages, 21488 KiB  
Article
Assessment of Early Glaucomatous Optic Neuropathy in the Dog by Spectral Domain Optical Coherence Tomography (SD-OCT)
by Annie Oh, Christine D. Harman, Kristin L. Koehl, Jiayan Huang, Leandro B. C. Teixeira, Laurence M. Occelli, Eric S. Storey, Gui-Shuang Ying and András M. Komáromy
Micromachines 2024, 15(6), 780; https://doi.org/10.3390/mi15060780 - 13 Jun 2024
Viewed by 205
Abstract
Background: Inherited primary open-angle glaucoma (POAG) in Beagle dogs is a well-established large animal model of glaucoma and is caused by a G661R missense mutation in the ADAMTS10 gene. Using this model, the study describes early clinical disease markers for canine glaucoma. Methods: [...] Read more.
Background: Inherited primary open-angle glaucoma (POAG) in Beagle dogs is a well-established large animal model of glaucoma and is caused by a G661R missense mutation in the ADAMTS10 gene. Using this model, the study describes early clinical disease markers for canine glaucoma. Methods: Spectral-domain optical coherence tomography (SD-OCT) was used to assess nine adult, ADAMTS10-mutant (median age 45.6 months, range 28.8–52.8 months; mean diurnal intraocular pressure (IOP): 29.9 +/− SEM 0.44 mmHg) and three related age-matched control Beagles (mean diurnal IOP: 18.0 +/− SEM 0.53 mmHg). Results: Of all the optic nerve head (ONH) parameters evaluated, the loss of myelin peak height in the horizontal plane was most significant (from 154 +/− SEM 38.4 μm to 9.3 +/− SEM 22.1 μm; p < 0.01). There was a strong significant negative correlation between myelin peak height and IOP (Spearman correlation: −0.78; p < 0.003). There were no significant differences in the thickness of any retinal layers evaluated. Conclusions: SD-OCT is a useful tool to detect early glaucomatous damage to the ONH in dogs before vision loss. Loss in myelin peak height without inner retinal thinning was identified as an early clinical disease marker. This suggests that initial degenerative changes are mostly due to the loss of myelin. Full article
(This article belongs to the Special Issue Optical Coherence Tomography (OCT) Technique and Its Applications)
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<p>Schematic diagram of spectral-domain optical coherence tomography (SD-OCT). Line charge-coupled device (CCD) detector. (Referenced from Zheng S et al. [<a href="#B26-micromachines-15-00780" class="html-bibr">26</a>]).</p>
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<p>Example of optic nerve head (ONH) measurements in a control dog. (<b>a</b>) cSLO image showing the location of the circular 12° OCT RNFL scan: ONH area (yellow shade); (<b>b</b>) cSLO image of a line scan: 0° (solid green line) and 90° (dashed green line) line scans; (<b>c</b>) Vitreoretinal reference plane (blue line): myelin peak height (yellow line) and ONH cup depth (green line). (<b>d</b>) Vitreoretinal reference plane (blue line): cross-sectional area of the ONH cup (green shade). (<b>e</b>) Neuroretinal rim reference plane (red line): myelin peak distance (length of red line) and ONH cup depth (purple line). (<b>f</b>) Neuroretinal rim reference plane (red line): cross-sectional area of the ONH cup (blue shade). Calibration bars = 200 μm.</p>
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<p>Example of optic nerve head (ONH) measurements in a control dog. (<b>a</b>) cSLO image showing the location of the 12 standard radial scans: four of these line scans were selected for measurements (white arrows; 0°, 45°, 90°, 135°). (<b>b</b>) Connected ends of the retinal pigment epithelium/choriocapillaris layer (blue line). One-hundred fifty micrometer reference plane (white line). Optic cup diameter (green line). Perpendicular lines from the ends of the retinal pigment epithelium/choriocapillaris layer to the inner limiting membrane (yellow lines). Cross-sectional neuroretinal rim area (red shade). Calibration bars = 200 μm.</p>
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<p>Example of retinal layer measurements in a control dog. (<b>a</b>) cSLO image of the 12° circular RNFL OCT scan: two distinct points per quadrant void of retinal blood vessels were identified. (<b>b</b>) FRT (red shade) extends from the ILM (red dots) to the RPE (purple dots). IRT (yellow shade) extends from the ILM (red dots) to the posterior surface of the IPL (yellow dots). ONL (green shade) is measured from its anterior (green dots) to the posterior surface (blue dots). Calibration bars = 200 μm.</p>
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<p>Scatterplot showing a significant negative correlation between intraocular pressure (IOP) and myelin peak height.</p>
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<p>Volume scans of three-dimensional SD-OCT images of the ONH. Two normal (<b>a</b>,<b>d</b>) and three affected ONHs (<b>b</b>,<b>c</b>,<b>e</b>) at various ages and stages of disease are shown. Right eye (OD); years old (YO).</p>
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<p>Histologic and SD-OCT comparison of the ONH. Normal (<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) and age-matched mutant Beagle dogs (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>). The 3.2-year-old and 3.3-year-old mutant dogs exhibit mild flattening of myelin on histology (<b>b</b>) and SD-OCT (<b>f</b>), respectively, in contrast to the 4.5-year-old mutant dog, which has marked myelin loss and cupping (arrows) of the ONH on both histology (<b>d</b>) and SD-OCT (<b>h</b>). Calibration bars = 200 μm. Right eye (OD); Left eye (OS); years old (YO).</p>
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<p>Histologic (superior retina) and SD-OCT (peripapillary) comparison of the retina. Normal (<b>a</b>,<b>c</b>,<b>e</b>,<b>g</b>) and age-matched mutant Beagle dogs (<b>b</b>,<b>d</b>,<b>f</b>,<b>h</b>). On histologic sections, there was thinning of the inner retina in the affected tissues (<b>b</b>,<b>d</b>) compared to age-matched controls (<b>a</b>,<b>c</b>) in both the early and later stages of the disease. This was not observed on SD-OCT when comparing the affected tissues (<b>f</b>,<b>h</b>) with age-matched controls (<b>e</b>,<b>f</b>) at the ages assessed. Calibration bars = 50 μm. Right eye (OD); Left eye (OS); years old (YO).</p>
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