[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
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
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
remove_circle_outline

Article Types

Countries / Regions

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Search Results (669)

Search Parameters:
Keywords = synthesis array

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
20 pages, 17778 KiB  
Article
Refining the Production Date of Historical Palestinian Garments Through Dye Identification
by Diego Tamburini, Ludovic Durand and Zeina Klink-Hoppe
Heritage 2025, 8(1), 28; https://doi.org/10.3390/heritage8010028 - 14 Jan 2025
Viewed by 430
Abstract
The dyes used to produce two Palestinian garments from the British Museum’s collection attributed to the late 19th–early 20th century were investigated by high pressure liquid chromatography coupled with diode array detector and tandem mass spectrometry (HPLC-DAD-MS/MS). Palestinian embroidery is a symbol of [...] Read more.
The dyes used to produce two Palestinian garments from the British Museum’s collection attributed to the late 19th–early 20th century were investigated by high pressure liquid chromatography coupled with diode array detector and tandem mass spectrometry (HPLC-DAD-MS/MS). Palestinian embroidery is a symbol of national identity and the topic of scholarly research. However, little attention has been given to the dyes and how these changed with the introduction of new synthetic formulations in the second half of the 19th century. The results revealed the use of natural indigoid blue and red madder (Rubia tinctorum), in combination with tannins. Yellow from buckthorn (probably Rhamnus saxatilis) and red from cochineal (probably Dactylopius coccus) were found mixed with synthetic dyes in green and dark red embroidery threads, respectively. Early synthetic dyes were identified in all the other colours. These include Rhodamine B (C.I. 45170), Orange II (C.I. 15510), Orange IV (C.I. 13080), Metanil Yellow (C.I. 13065), Chrysoidine R (C.I. 11320), Methyl Violet (C.I. 42535), Malachite Green (C.I. 42000), Fuchsin (C.I. 42510), Auramine O (C.I. 41000) and Methyl Blue (C.I. 42780). As the date of the first synthesis of these dyes is known, the production date of the garments was refined, suggesting that these were likely to be produced towards the end of the 1880s/beginning of the 1890s. The continuous use of historical local sources of natural dyes, alongside new synthetic dyes, is of particular interest, adding rightful nuances to the development of textile-making practices in this region. Full article
(This article belongs to the Special Issue Dyes in History and Archaeology 43)
Show Figures

Figure 1

Figure 1
<p>Front, back and details of the embroidery of As1967,02.15 (length: 129 cm; width: 103 cm). Light blue rectangles indicate the discoloured red areas. ©The Trustees of the British Museum.</p>
Full article ">Figure 2
<p>Front, back and details of the embroidery and appliqués of As1967,02.21 (length: 132 cm; width: 94 cm). ©The Trustees of the British Museum.</p>
Full article ">Figure 3
<p>Extracted ion chromatograms obtained by HPLC-MS analysis of (<b>a</b>) non-faded red, (<b>b</b>) faded red and (<b>c</b>) dark red samples from As1967,02.15. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 4
<p>Results obtained for the orange sample from As1967,02.15: (<b>a</b>) UV-Vis chromatogram extracted at 450 nm and absorption spectra (insets) of the two molecules; (<b>b</b>) extracted ion chromatograms of ions [M-H]<sup>−</sup> = 327.045 <span class="html-italic">m</span>/<span class="html-italic">z</span> and 352.076 <span class="html-italic">m</span>/<span class="html-italic">z</span>; (<b>c</b>,<b>d</b>) corresponding tandem mass spectra (CID = 30 eV). For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 5
<p>Results obtained for the yellow sample from As1967,02.15: (<b>a</b>) UV-Vis chromatogram extracted at 450 nm and absorption spectrum (insets) of Metanil Yellow; (<b>b</b>) extracted ion chromatograms of ions [M-H]<sup>−</sup> = 327.045 <span class="html-italic">m</span>/<span class="html-italic">z</span> and 352.076 <span class="html-italic">m</span>/<span class="html-italic">z</span> and ion [M]<sup>+</sup> = 237.114 <span class="html-italic">m</span>/<span class="html-italic">z</span>; (<b>c</b>,<b>d</b>) tandem mass spectra (CID = 30 eV) of Metanil Yellow and Chrysoidine R degradation product. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 6
<p>Conversion of Chrysoidine R into its degradation product.</p>
Full article ">Figure 7
<p>Results obtained for the yellow sample from As1967,02.21: (<b>a</b>) UV-Vis chromatograms extracted at 350, 450 and 600 nm; (<b>b</b>) extracted ion chromatograms of ions corresponding to the flavonoid components of <span class="html-italic">Rhamnus</span> sp. and molecular structure of rhamnazin-3-O-rhamninoside. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 8
<p>Extracted ion chromatograms in (<b>a</b>) negative and (<b>b</b>) positive ionisation modes, obtained by HPLC-MS analysis of the green sample from As1967,02.15. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 9
<p>Extracted ion chromatograms obtained by HPLC-MS analysis of (<b>a</b>) purple and (<b>b</b>) bright pink samples from As1967,02.15. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">Figure 10
<p>Results obtained for the light blue sample from As1967,02.21: (<b>a</b>) UV-Vis chromatogram extracted at 600 nm; (<b>b</b>) extracted ion chromatograms of ions corresponding to the molecular components of Methyl Blue. For peak labels and molecular details, see <a href="#heritage-08-00028-t003" class="html-table">Table 3</a>. ©The Trustees of the British Museum.</p>
Full article ">
25 pages, 4089 KiB  
Article
Taguchi Method-Based Synthesis of a Circular Antenna Array for Enhanced IoT Applications
by Wided Amara, Ramzi Kheder, Ridha Ghayoula, Issam El Gmati, Amor Smida, Jaouhar Fattahi and Lassaad Latrach
Telecom 2025, 6(1), 7; https://doi.org/10.3390/telecom6010007 - 14 Jan 2025
Viewed by 326
Abstract
Linear antenna arrays exhibit radiation patterns that are restricted to a half-space and feature axial radiation, which can be a significant drawback for applications that require omnidirectional coverage. To address this limitation, the synthesis method utilizing the Taguchi approach, originally designed for linear [...] Read more.
Linear antenna arrays exhibit radiation patterns that are restricted to a half-space and feature axial radiation, which can be a significant drawback for applications that require omnidirectional coverage. To address this limitation, the synthesis method utilizing the Taguchi approach, originally designed for linear arrays, can be effectively extended to two-dimensional or planar antenna arrays. In the context of a linear array, the synthesis process primarily involves determining the feeding law and/or the spatial distribution of the elements along a single axis. Conversely, for a planar array, the synthesis becomes more complex, as it requires the identification of the complex weighting of the feed and/or the spatial distribution of sources across a two-dimensional plane. This adaptation to planar arrays is facilitated by substituting the direction θ with the pair of directions (θ,ϕ), allowing for a more comprehensive coverage of the angular domain. This article focuses on exploring various configurations of planar arrays, aiming to enhance their performance. The primary objective of these configurations is often to minimize the levels of secondary lobes and/or array lobes while enabling a full sweep of the angular space. Secondary lobes can significantly impede system performance, particularly in multibeam applications, where they restrict the minimum distance for frequency channel reuse. This restriction is critical, as it affects the overall efficiency and effectiveness of communication systems that rely on precise beamforming and frequency allocation. By investigating alternative planar array designs and their synthesis methods, this research seeks to provide solutions that improve coverage, reduce interference from secondary lobes, and ultimately enhance the functionality of antennas in diverse applications, including telecommunications, radar systems, and wireless communication. Full article
Show Figures

Figure 1

Figure 1
<p>Electronic-scanning of the space with a secondary lobe level of −8 dB for a circular antenna array of 24 elements.</p>
Full article ">Figure 2
<p>Electronic-scanning of the space with a secondary lobe level of −28 dB for a circular antenna array of 16 elements.</p>
Full article ">Figure 3
<p>Geometry of the proposed antenna.</p>
Full article ">Figure 4
<p>Design and simulation of a circular antenna array with 10 elements.</p>
Full article ">Figure 5
<p>Reflection coefficient of the proposed antenna and 3D radiation pattern at 2.45 GHz.</p>
Full article ">Figure 6
<p>Polar radiation patterns for a circular antenna array with 10-elements at 2.45 GHz.</p>
Full article ">Figure 7
<p>Simulated results for 3D circular antenna array radiation pattern synthesis with 10-elements using PSO and GA algorithms at 2.45 GHz.</p>
Full article ">Figure 8
<p>Circular antenna array with 16-elements at 2.45 GHz. (<b>a</b>) Uniform excitation (16 antennas). (<b>b</b>) Taguchi excitation (16 antennas).</p>
Full article ">Figure 9
<p>Circular antenna array with 24-elements at 2.45 GHz. (<b>a</b>) Uniform excitation (24-antennas). (<b>b</b>) Taguchi excitation (24-antennas).</p>
Full article ">Figure 10
<p>Circular antenna array in concentric rings with isotropic elements.</p>
Full article ">Figure 11
<p>Simulation results of a concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>2</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 12
<p>Simulation results of a concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 13
<p>Simulation results of a concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 14
<p>Simulation results of a concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 15
<p>Simulation results of a concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>4</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>).</p>
Full article ">Figure 16
<p>Reduction of the side-lobe level for concentric ring arrays.</p>
Full article ">Figure 17
<p>Optimal excitation values found using the Taguchi method.</p>
Full article ">Figure 18
<p>Synthesis of 3D radiation patterns for an 18-element array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>) at 2.45 GHz. (<b>a</b>) Structure of the concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>4</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>). (<b>b</b>) Uniform excitations. (<b>c</b>) Excitations with Evolutionary Programming (EP). (<b>d</b>) Excitations with Firefly Algorithm (FA). (<b>e</b>) Excitations with Taguchi method.</p>
Full article ">Figure 19
<p>Synthesis of 3D radiation patterns for a 24-element array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>) at 2.45 GHz. (<b>a</b>) Structure of the concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>). (<b>b</b>) Uniform excitations. (<b>c</b>) Excitations with Taguchi method.</p>
Full article ">Figure 20
<p>Synthesis of 3D radiation patterns for a 30-element array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>) at 2.45 GHz. (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>), (<b>a</b>) Structure of the concentric ring array and (<b>b</b>) Uniform excitations. (<b>c</b>) Excitations with Evolutionary Programming (EP). (<b>d</b>) Excitations with the Firefly Algorithm (FA). (<b>e</b>) Excitations with Taguchi.</p>
Full article ">Figure 21
<p>Synthesis of 3D radiation patterns for a 36-element array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>4</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>) at <math display="inline"><semantics> <mrow> <mn>2.45</mn> </mrow> </semantics></math> GHz. (<b>a</b>) Structure of the concentric ring array (<math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>1</mn> </msub> <mo>=</mo> <mn>6</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>8</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>3</mn> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mi>N</mi> <mn>4</mn> </msub> <mo>=</mo> <mn>12</mn> </mrow> </semantics></math>). (<b>b</b>) Uniform excitations. (<b>c</b>) Excitations with Taguchi optimization.</p>
Full article ">
18 pages, 5416 KiB  
Article
Bacteria-Inspired Synthesis of Silver-Doped Zinc Oxide Nanocomposites: A Novel Synergistic Approach in Controlling Biofilm and Quorum-Sensing-Regulated Virulence Factors in Pseudomonas aeruginosa
by Abirami Karthikeyan, Manoj Kumar Thirugnanasambantham, Fazlurrahman Khan and Arun Kumar Mani
Antibiotics 2025, 14(1), 59; https://doi.org/10.3390/antibiotics14010059 - 9 Jan 2025
Viewed by 529
Abstract
Multidrug-resistant Pseudomonas aeruginosa infections pose a critical challenge to healthcare systems, particularly in nosocomial settings. This drug-resistant bacterium forms biofilms and produces an array of virulent factors regulated by quorum sensing. In this study, metal-tolerant bacteria were isolated from a metal-contaminated site and [...] Read more.
Multidrug-resistant Pseudomonas aeruginosa infections pose a critical challenge to healthcare systems, particularly in nosocomial settings. This drug-resistant bacterium forms biofilms and produces an array of virulent factors regulated by quorum sensing. In this study, metal-tolerant bacteria were isolated from a metal-contaminated site and screened for their ability to synthesize multifunctional nanocomposites (NCs). Rapid color changes in the reaction solution evidenced the biotransformation process. The potent isolated Bacillus cereus SASAK, identified via 16S rRNA sequencing and deposited in GenBank under accession number MH885570, facilitated the microbial-mediated synthesis of ZnO nanoparticles and silver-doped ZnO NCs. These biogenic nanocomposites were characterized using UV-VIS-NIR spectroscopy, FTIR, XRD, zeta potential, HRTEM, FESEM, and EDX analyses. At a sub-MIC concentration of 100 µg/mL, 2% Ag-ZnO NCs effectively inhibited virulent factor production and biofilm formation in P. aeruginosa without affecting bacterial growth. Notably, there was a significant reduction in violacein pigment (96.25%), swarming motility, and pyocyanin concentration (1.87 µg/mL). Additionally, biofilm formation (81.1%) and EPS production (83.9%) using P. aeruginosa were substantially hindered, along with reduced extracellular protease activity, as indicated by zone formation (from 2.3 to 1.8 cm). This study underscores the potential of Ag-ZnO NCs as promising agents for combating quorum sensing-mediated virulence in chronic infections caused by multidrug-resistant P. aeruginosa. Full article
(This article belongs to the Special Issue Antimicrobial Resistance in Biofilm-Associated Infections)
Show Figures

Figure 1

Figure 1
<p>Screening and molecular identification of potent bacterial strain for the synthesis of Ag-ZnO NCs. (<b>A</b>) Screening of isolated bacteria (SASAK) for the synthesis of Ag-ZnO NCs and bacterial-inspired synthesis of Ag-ZnO NCs, (<b>B</b>) initial color change, (<b>C</b>) final color change, and (<b>D</b>) phylogenetic tree of isolated bacteria (<span class="html-italic">Bacillus cereus</span> SASAK).</p>
Full article ">Figure 2
<p>UV-vis NIR spectrum of undoped ZnO NPs and Ag-ZnO NCs. (<b>A</b>) Bandgap spectra and (<b>B</b>) UV-vis absorption spectra.</p>
Full article ">Figure 3
<p>Characterization of NCs (<b>A</b>). Histogram showing the particle size analysis of 2% Ag-ZnO NCs, (<b>B</b>) the zeta potential distributions of 2% Ag-ZnO NCs, (<b>C</b>) the XRD spectra of undoped ZnO NPs and Ag-ZnO NCs, and (<b>D</b>) the FTIR spectrum of undoped ZnO NPs and Ag-ZnO NCs.</p>
Full article ">Figure 4
<p>Morphological and elemental composition of 2% Ag-ZnO NCs (<b>A</b>). FESEM analysis (<b>B</b>) and (<b>C</b>) size analysis of NCs using HRTEM, and (<b>D</b>) EDX analysis of NCs.</p>
Full article ">Figure 5
<p>(<b>A</b>) Antibiotic susceptibility test against the hospital-acquired test pathogen <span class="html-italic">P. aeruginosa</span>; (<b>B</b>) the effect of pure and Ag-ZnO NCs on the cell viability of <span class="html-italic">P. aeruginosa</span>; and (<b>C</b>) the determination of the MIC and sub-MIC of 2% Ag-ZnO NCs, including the positive control (without NCs) and negative control (0.5 µg/mL of colistin).</p>
Full article ">Figure 6
<p>Antiquorum sensing activity of NCs. (<b>A</b>) The inhibition of the violacein pigment in bioreporter strain <span class="html-italic">C. violaceum</span> using 2% Ag-ZnO NCs, (<b>B</b>) the pyocyanin inhibition assay, and (<b>C</b>) the inhibition of biofilm formation using undoped ZnO NPs and 2% Ag-ZnO NCs using the Congo red assay and tube assay, and (<b>D</b>) the inhibition of EPSs using undoped ZnO NPs and 2% Ag-ZnO NCs.</p>
Full article ">Figure 7
<p>(<b>A</b>) The inhibition of swarming motility and (<b>B</b>) protease inhibition assay.</p>
Full article ">
14 pages, 2978 KiB  
Communication
In Situ Synthesis of Ternary Ni-Fe-Mo Nanosheet Arrays for OER in Water Electrolysis
by Zhi Lu, Yifan Guo, Shilin Li, Jiaqi Ding, Yingzi Ren, Kun Tang, Jiefeng Wang, Chengxin Li, Zishuo Shi, Ziqi Sun, Hongbo Meng and Guangxin Wang
Molecules 2025, 30(1), 177; https://doi.org/10.3390/molecules30010177 - 4 Jan 2025
Viewed by 645
Abstract
Water electrolysis is a promising path to the industrialization development of hydrogen energy. The exploitation of high-efficiency and inexpensive catalysts become important to the mass use of water decomposition. Ni-based nanomaterials have exhibited great potential for the catalysis of water splitting, which have [...] Read more.
Water electrolysis is a promising path to the industrialization development of hydrogen energy. The exploitation of high-efficiency and inexpensive catalysts become important to the mass use of water decomposition. Ni-based nanomaterials have exhibited great potential for the catalysis of water splitting, which have attracted the attention of researchers around the world. Here, we prepared a novel Mo-doped NiFe-based layered double hydroxide (LDH) with a nanoarray microstructure on Ni foam. The doping amount of Mo can significantly change the microstructure of the electrocatalysis, which will further affect the oxygen evolution reaction (OER) performance of water splitting. This novel nanomaterial required only an overpotential of 227 mV for 10 mA cm−2 and a Tafel slope of 54.8 mV/dec in 1 M KOH. Meanwhile, there was no Mo, and the NiFe-LDH needed 233 mV to attain to 10 mA cm−2. Compared to the NiFe-LDH without Mo, the NiFeMo-LDH nanosheet arrays exhibited enhanced activities with 17.1 mV/dec less Tafel in OER. The good performance of the electrocatalyst is ascribed to the special nanosheet arrays and the heterostructure of the Ni-Fe-Mo system. These features help to increase the active surface, enhancing the efficient charge transfer and the reactive activity in OER. Full article
(This article belongs to the Topic Fabrication of Hybrid Materials for Catalysis)
Show Figures

Figure 1

Figure 1
<p>SEM of (<b>a1</b>,<b>a2</b>) pre-treated NF and (<b>b1</b>,<b>b2</b>) the surface after synthesis. Macro-scale images of (<b>c1</b>) NiFe-LDH/NF, (<b>d1</b>) NiFeMo<sub>0.1</sub>-LDH/NF, (<b>e1</b>) NiFeMo<sub>0.2</sub>-LDH, (<b>f1</b>) NiFeMo<sub>0.3</sub>-LDH nanosheet arrays. High magnification of (<b>c2</b>) NiFe-LDH/NF, (<b>d2</b>) NiFeMo<sub>0.1</sub>-LDH/NF, (<b>e2</b>) NiFeMo<sub>0.2</sub>-LDH, (<b>f2</b>) NiFeMo<sub>0.3</sub>-LDH.</p>
Full article ">Figure 2
<p>XRD patterns of NiFeMo-based LDH. The patterns of NiFe-LDH (black), NiFeMo<sub>0.1</sub>-LDH (red), NiFeMo<sub>0.2</sub>-LDH (blue) and NiFeMo<sub>0.3</sub>-LDH (green).</p>
Full article ">Figure 3
<p>(<b>a</b>) TEM morphology, (<b>b</b>) SAED, (<b>c</b>) high-resolution image of NiFeMo<sub>0.1</sub>-LDH.</p>
Full article ">Figure 4
<p>EDS of NiFeMo<sub>0.1</sub>-LDH nanosheet arrays. (<b>a</b>) SEM of NiFeMo<sub>0.1</sub>-LDH; the distribution of (<b>b</b>) Ni, (<b>c</b>) O, (<b>d</b>) Fe, (<b>e</b>) Mo, (<b>f</b>) EDS of NiFeMo<sub>0.1</sub>-LDH surface.</p>
Full article ">Figure 5
<p>XPS of (<b>a</b>) survey spectrum, (<b>b</b>) Ni 2p, (<b>c</b>) Fe 2p, (<b>d</b>) Mo 3d of NiFeMo<sub>0.1</sub>-LDH. The red curves are the fitted curves of test data, the dark green and purple curves are the peaks of the main elements, the light green and yellow curves are the satellite peaks, the blue curves are the baseline of the fitted curves.</p>
Full article ">Figure 6
<p>(<b>a</b>) LSV curves at 2 mVs<sup>−1</sup>. (<b>b</b>) Tafel slopes. (<b>c</b>) C<sub>dl</sub> curves. (<b>d</b>) EIS with the equivalent circuit.</p>
Full article ">Figure 7
<p>Stability test of the NiFeMo<sub>0.1</sub>-LDH nanosheet arrays.</p>
Full article ">Figure 8
<p>(<b>a</b>) LSV curves of NiFeMo<sub>0.1</sub>-LDH in stability test. (<b>b</b>) Morphology of NiFeMo<sub>0.1</sub>-LDH after OER.</p>
Full article ">
17 pages, 320 KiB  
Article
Effect of Genetic Variants on Rosuvastatin Pharmacokinetics in Healthy Volunteers: Involvement of ABCG2, SLCO1B1 and NAT2
by Eva González-Iglesias, Clara Méndez-Ponce, Dolores Ochoa, Manuel Román, Gina Mejía-Abril, Samuel Martín-Vilchez, Alejandro de Miguel, Antía Gómez-Fernández, Andrea Rodríguez-Lopez, Paula Soria-Chacartegui, Francisco Abad-Santos and Jesús Novalbos
Int. J. Mol. Sci. 2025, 26(1), 260; https://doi.org/10.3390/ijms26010260 - 30 Dec 2024
Viewed by 595
Abstract
Statins are the primary drugs used to prevent cardiovascular disease by inhibiting the HMG-CoA reductase, an enzyme crucial for the synthesis of LDL cholesterol in the liver. A significant number of patients experience adverse drug reactions (ADRs), particularly musculoskeletal problems, which can affect [...] Read more.
Statins are the primary drugs used to prevent cardiovascular disease by inhibiting the HMG-CoA reductase, an enzyme crucial for the synthesis of LDL cholesterol in the liver. A significant number of patients experience adverse drug reactions (ADRs), particularly musculoskeletal problems, which can affect adherence to treatment. Recent clinical guidelines, such as those from the Clinical Pharmacogenetics Implementation Consortium (CPIC) in 2022, recommend adjusting rosuvastatin doses based on genetic variations in the ABCG2 and SLCO1B1 genes to minimize ADRs and improve treatment efficacy. Despite these adjustments, some patients still experience ADRs. So, we performed a candidate gene study to better understand the pharmacogenetics of rosuvastatin. This study included 119 healthy volunteers who participated in three bioequivalence trials of rosuvastatin alone or in combination with ezetimibe at the Clinical Trials Unit of the Hospital Universitario de La Princesa (UECHUP). Participants were genotyped using a custom OpenArray from ThermoFisher that assessed 124 variants in 38 genes associated with drug metabolism and transport. No significant differences were observed according to sex or biogeographic origin. A significant increase in t1/2 (pmultivariate(pmv) = 0.013) was observed in the rosuvastatin plus ezetimibe trial compared with the rosuvastatin alone trials. Genetic analysis showed that decreased (DF) and poor function (PF) volunteers for the ABCG2 transporter had higher AUC/DW (adjusted dose/weight), AUC72h/DW and Cmax/DW compared to normal function (NF) volunteers (pmv< 0.001). DF and PF volunteers for SLCO1B1 showed an increase in AUC72h/DW (pmv = 0.020) compared to increased (IF) and NF individuals. Results for ABCG2 and SLCO1B1 were consistent with the existing literature. In addition, AUC/DW, AUC72h/DW and Cmax/DW were increased in intermediate (IA) and poor (PA) NAT2 acetylators (pmv = 0.001, pmv< 0.001, pmv< 0.001, respectively) compared to rapid acetylators (RA), which could be associated through a secondary pathway that was previously unknown. Full article
(This article belongs to the Special Issue Advancements in Diagnostic and Preventive Pharmacogenomics)
18 pages, 3376 KiB  
Article
Heterogeneous Edge Computing for Molecular Property Prediction with Graph Convolutional Networks
by Mahdieh Grailoo and Jose Nunez-Yanez
Electronics 2025, 14(1), 101; https://doi.org/10.3390/electronics14010101 - 30 Dec 2024
Viewed by 457
Abstract
Graph-based neural networks have proven to be useful in molecular property prediction, a critical component of computer-aided drug discovery. In this application, in response to the growing demand for improved computational efficiency and localized edge processing, this paper introduces a novel approach that [...] Read more.
Graph-based neural networks have proven to be useful in molecular property prediction, a critical component of computer-aided drug discovery. In this application, in response to the growing demand for improved computational efficiency and localized edge processing, this paper introduces a novel approach that leverages specialized accelerators on a heterogeneous edge computing platform. Our focus is on graph convolutional networks, a leading graph-based neural network variant that integrates graph convolution layers with multi-layer perceptrons. Molecular graphs are typically characterized by a low number of nodes, leading to low-dimensional dense matrix multiplications within multi-layer perceptrons—conditions that are particularly well-suited for Edge TPUs. These TPUs feature a systolic array of multiply–accumulate units optimized for dense matrix operations. Furthermore, the inherent sparsity in molecular graph adjacency matrices offers additional opportunities for computational optimization. To capitalize on this, we developed an FPGA GFADES accelerator, using high-level synthesis, specifically tailored to efficiently manage the sparsity in both the graph structure and node features. Our hardware/software co-designed GCN+MLP architecture delivers performance improvements, achieving up to 58× increased speed compared to conventional software implementations. This architecture is implemented using the Pynq framework and TensorFlow Lite Runtime, running on a multi-core ARM CPU within an AMD/Xilinx Zynq Ultrascale+ device, in combination with the Edge TPU and programmable logic. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) ML architecture for molecular property prediction, including 3-layer GCNs and 2-layer MLP. (<b>b</b>) Heterogeneous architecture, incorporating ARM CPU, FPGA, and Edge TPU, tailored to the nature of computations.</p>
Full article ">Figure 2
<p>(<b>a</b>) Molecular graph representations. (<b>b</b>) Adjacency and node matrix dimensions, accounting for the impact of batch size <math display="inline"> <semantics> <mrow> <mi>b</mi> <mi>z</mi> </mrow> </semantics> </math>.</p>
Full article ">Figure 3
<p>Runtime Analysis of GCN+MLP architecture on the Zynq UltraScale+ MPSoC ZCU102 Board for MUTAG, NCI1, PROTEINS, and ENZYMES datasets: (CPU) demonstrates the runtime dominance of sparse/dense × dense matrix operations within three GCN layers (GCN1, GCN2, GCN3) in full software implementations; (CPU+FPGA) highlights the runtime bottleneck of the software 2-layer MLP.</p>
Full article ">Figure 4
<p>FPGA GFADES GCN/ReLU accelerator, incorporating multi-threaded hardware GCN accelerator configured with 4 combination threads, 4 aggregation threads, and 4 compute cores per thread (4t4t4c) setup.</p>
Full article ">Figure 5
<p>Vivado block diagram depicting the architectural design.</p>
Full article ">Figure 6
<p>The operational test stand showing the module connections within the system and its real-time behavior.</p>
Full article ">Figure 7
<p>Comparative analysis of runtime speedups across various layers/networks and the full GCN+MLP architecture using FPGA GFADES and Edge TPU accelerators for the various datasets.</p>
Full article ">Figure 8
<p>Comparative analysis of runtime speedups across various batch sizes during inference phase on CPU+FPGA+TPU for the various datasets.</p>
Full article ">Figure 9
<p>Resource utilization of the FPGA GFADES GCN accelerators (GCN/ReLU in 4t4t4c), design power distribution for implemented netlist, and design timing of the designed architecture.</p>
Full article ">
14 pages, 495 KiB  
Article
Recurrent Deep Learning for Beam Pattern Synthesis in Optimized Antenna Arrays
by Armando Arce, Fernando Arce, Enrique Stevens-Navarro, Ulises Pineda-Rico, Marco Cardenas-Juarez and Abel Garcia-Barrientos
Appl. Sci. 2025, 15(1), 204; https://doi.org/10.3390/app15010204 - 29 Dec 2024
Viewed by 650
Abstract
This work proposes and describes a deep learning-based approach utilizing recurrent neural networks (RNNs) for beam pattern synthesis considering uniform linear arrays. In this particular case, the deep neural network (DNN) learns from previously optimized radiation patterns as inputs and generates complex excitations [...] Read more.
This work proposes and describes a deep learning-based approach utilizing recurrent neural networks (RNNs) for beam pattern synthesis considering uniform linear arrays. In this particular case, the deep neural network (DNN) learns from previously optimized radiation patterns as inputs and generates complex excitations as output. Beam patterns are optimized using a genetic algorithm during the training phase in order to reduce sidelobes and achieve high directivity. Idealized and test beam patterns are employed as inputs for the DNN, demonstrating their effectiveness in scenarios with high prediction complexity and closely spaced elements. Additionally, a comparative analysis is conducted among the three DNN architectures. Numerical experiments reveal improvements in performance when using the long short-term memory network (LSTM) compared to fully connected and convolutional neural networks. Full article
Show Figures

Figure 1

Figure 1
<p>Proposed deep neural network architectures for prediction of the amplitude and phase of radiation patterns. (<b>a</b>) FCNN composed of four fully connected layers with 128 ReLU neurons and an output layer composed of 16 linear neurons. (<b>b</b>) 1D-CNN made up of two 1D-convolutional layers with 1024 and 512 hyperbolic tangent activation functions, two fully connected layers with 128 ReLU neurons, and an output layer of 16 linear neurons. (<b>c</b>) LSTM built using two LSTM layers with 1024 and 512 hyperbolic tangent activation functions, two fully connected layers with 128 ReLU neurons, and an output layer consisting of 16 linear neurons.</p>
Full article ">Figure 2
<p>Uniform linear array of 8 antenna elements used as a case study.</p>
Full article ">Figure 3
<p>Example of normalized power pattern ranging from 1 to 180 degrees.</p>
Full article ">Figure 4
<p>Performance of the LSTM during training and validation. (<b>a</b>) MSE during the training and validation process. (<b>b</b>) MAE during the training and validation process.</p>
Full article ">Figure 5
<p>Synthesized beam patterns obtained with idealized inputs: (<b>a</b>) Arbitrary triangular pulse and (<b>b</b>) arbitrary square.</p>
Full article ">Figure 6
<p>Radiation pattern synthesis resulting from test input patterns: (<b>a</b>) Test pattern 1 and (<b>b</b>) test pattern 2.</p>
Full article ">Figure 7
<p>Beam pattern synthesis obtained from input patterns with mutual coupling: (<b>a</b>) Test pattern at 65° and (<b>b</b>) test pattern at 115°.</p>
Full article ">
21 pages, 1104 KiB  
Article
Advancing Applications of Robot Audition Systems: Efficient HARK Deployment with GPU and FPGA Implementations
by Zirui Lin, Hideharu Amano, Masayuki Takigahira, Naoya Terakado, Katsutoshi Itoyama, Haris Gulzar and Kazuhiro Nakadai
Chips 2025, 4(1), 2; https://doi.org/10.3390/chips4010002 - 27 Dec 2024
Viewed by 400
Abstract
This paper proposes efficient implementations of robot audition systems, specifically focusing on deployments using HARK, an open-source software (OSS) platform designed for robot audition. Although robot audition systems are versatile and suitable for various scenarios, efficiently deploying them can be challenging due to [...] Read more.
This paper proposes efficient implementations of robot audition systems, specifically focusing on deployments using HARK, an open-source software (OSS) platform designed for robot audition. Although robot audition systems are versatile and suitable for various scenarios, efficiently deploying them can be challenging due to their high computational demands and extensive processing times. For scenarios involving intensive high-dimensional data processing with large-scale microphone arrays, our generalizable GPU-based implementation significantly reduced processing time, enabling real-time Sound Source Localization (SSL) and Sound Source Separation (SSS) using a 60-channel microphone array across two distinct GPU platforms. Specifically, our implementation achieved speedups of 23.3× for SSL and 3.0× for SSS on a high-performance server equipped with an NVIDIA A100 80 GB GPU. Additionally, on the Jetson AGX Orin 32 GB, which represents embedded environments, it achieved speedups of 14.8× for SSL and 1.6× for SSS. For edge computing scenarios, we developed an adaptable FPGA-based implementation of HARK using High-Level Synthesis (HLS) on M-KUBOS, a Multi-Access Edge Computing (MEC) FPGA Multiprocessor System on a Chip (MPSoC) device. Utilizing an eight-channel microphone array, this implementation achieved a 1.2× speedup for SSL and a 1.1× speedup for SSS, along with a 1.1× improvement in overall energy efficiency. Full article
Show Figures

Figure 1

Figure 1
<p>Online batch processing flow of HARK for sound source localization (SSL) and sound source separation (SSS) tasks using its Python interface, PyHARK.</p>
Full article ">Figure 2
<p>Architecture of the SSL implementation.</p>
Full article ">Figure 3
<p>Microphone arrays utilized in evaluations.</p>
Full article ">Figure 4
<p>Resource usage of FPGA-based implementation.</p>
Full article ">Figure 5
<p>Experimental setup for audio data acquisition.</p>
Full article ">Figure 6
<p>Total average processing time for SSL and SSS for each second of 60-channel audio on different processors. Bars below the threshold indicate real-time capability, while bars above the threshold do not meet real-time requirements.</p>
Full article ">
10 pages, 3764 KiB  
Article
Synthesis of the Large-Scaled 64 × 64 Thinned Array Using the Branch and Bound Technique with Convex Optimization for Satellite Communication
by Xuelian Li, Yan Wang and Chuansong Zhang
Electronics 2025, 14(1), 23; https://doi.org/10.3390/electronics14010023 - 25 Dec 2024
Viewed by 316
Abstract
This paper presents the synthesis of a 64 × 64 thinned array, using the branch and bound technique with convex optimization and a low sidelobe level for satellite communication. The branch and bound technology decomposes optimization into several subproblems. The convex optimization transforms [...] Read more.
This paper presents the synthesis of a 64 × 64 thinned array, using the branch and bound technique with convex optimization and a low sidelobe level for satellite communication. The branch and bound technology decomposes optimization into several subproblems. The convex optimization transforms the optimized variable binary [0, 1] of the thinned array into a continuous variable, i.e., from 0 to 1. Based on the branch and bound technique with convex optimization, the fast and accurate convergence of the synthesis of large-scale thinned array was achieved, and 2400 elements were selected for a full 64 × 64 array with a sidelobe level that satisfies the system requirements. The proposed thinned array with 2400 elements was simulated via full-wave 3D simulation. A prototype of the proposed thinned array was fabricated and measured. The simulated and measured results verified the effectiveness of the branch and bound technique with convex optimization. Full article
(This article belongs to the Special Issue Antenna and Array Design for Future Sensing and Communication System)
Show Figures

Figure 1

Figure 1
<p>Three-dimensional view of the full 64 × 64 array. (<b>a</b>) The full 64 × 64 array. (<b>b</b>) The full 32 × 32 array with a 2 × 2 subarray.</p>
Full article ">Figure 2
<p>Array structure and array element of the proposed thinned array. (<b>a</b>) Structure of the thinned array with 2400 elements (the “red box” represents the active element, and the “white box” represents no elements). (<b>b</b>) Structure of the array element: (<b>b1</b>) side view, (<b>b2</b>) top view of Sub1, and (<b>b3</b>) top view of Sub2; <span class="html-italic">h</span>1 = 0.381, <span class="html-italic">h</span>2 = 0.381, <span class="html-italic">h</span>3 = 0.1 mm, <span class="html-italic">h</span>4 = 0.203, <span class="html-italic">Lp</span>1 = 2.4, <span class="html-italic">Lp</span>2 = 2.6, <span class="html-italic">Lg</span> = 5, units: mm. (<b>c</b>) Model of the proposed thinned array with 2400 elements and an element spacing of 5 mm. (<b>d</b>) Fabricated prototype of the proposed thinned array with 2400 elements. (<b>e</b>) Top-down view of the bottom-right quarter of the array. (<b>f</b>) Bottom-up view of bottom-right quarter of the array.</p>
Full article ">Figure 3
<p>Simulated S-parameters of the array element in the cases of single element (<a href="#electronics-14-00023-f002" class="html-fig">Figure 2</a>b) and in the array (<a href="#electronics-14-00023-f002" class="html-fig">Figure 2</a>c).</p>
Full article ">Figure 4
<p>Simulated radiation patterns of the array element in the cases of single element (<a href="#electronics-14-00023-f002" class="html-fig">Figure 2</a>b) and in the array (<a href="#electronics-14-00023-f002" class="html-fig">Figure 2</a>c) at 29 GHz. (<b>a</b>) E-plane (<span class="html-italic">xz</span>-plane). (<b>b</b>) H-plane (<span class="html-italic">yz</span>-plane).</p>
Full article ">Figure 5
<p>Two-dimensional normalized array factor of the large-scale sparse array with 2400 elements. (<b>a</b>) <span class="html-italic">φ</span> = 0° cut-plane. (<b>b</b>) <span class="html-italic">φ</span> = 45° cut-plane. (<b>c</b>) <span class="html-italic">φ</span> = 90° cut-plane. (<b>d</b>) <span class="html-italic">φ</span> = 135° cut-plane.</p>
Full article ">Figure 6
<p>Three-dimensional normalized array factor of the large-scale thinned array with 2400 elements.</p>
Full article ">Figure 7
<p>Simulated 3D radiation patterns of the thinned array.</p>
Full article ">Figure 8
<p>Simulated and measured normalized radiation patterns of the thinned array in the <span class="html-italic">φ</span> = 0° and <span class="html-italic">φ</span> = 45° cut-planes. (<b>a</b>) <span class="html-italic">φ</span> = 0° cut-plane. (<b>b</b>) <span class="html-italic">φ</span> = 45° cut-plane.</p>
Full article ">
18 pages, 14199 KiB  
Article
Enhanced Virtual Sound Source Construction Based on Wave Field Synthesis Using Crossfade Processing with Electro-Dynamic and Parametric Loudspeaker Arrays
by Yuting Geng, Ayano Hirose, Mizuki Iwagami, Masato Nakayama and Takanobu Nishiura
Appl. Sci. 2024, 14(24), 11911; https://doi.org/10.3390/app142411911 - 19 Dec 2024
Viewed by 465
Abstract
Wave field synthesis (WFS) can be used to construct virtual sound sources (VSSs) with a loudspeaker array. Conventional methods using a single type of loudspeaker showed limited performance in distance perception. For example, WFS with electro-dynamic loudspeakers (EDLs) has the advantage of constructing [...] Read more.
Wave field synthesis (WFS) can be used to construct virtual sound sources (VSSs) with a loudspeaker array. Conventional methods using a single type of loudspeaker showed limited performance in distance perception. For example, WFS with electro-dynamic loudspeakers (EDLs) has the advantage of constructing VSSs near the loudspeaker, while WFS with parametric array loudspeakers (PALs) has the advantage of constructing VSSs far from the loudspeaker. In this paper, we propose a VSS construction method utilizing crossfade processing with both EDLs and PALs. The contribution of EDLs and PALs was balanced to better synthesize the target sound field. We carried out experiments to evaluate the sound pressure, frequency characteristic, and sound image perception. The experimental results demonstrated that the proposed method can enhance these aspects of the VSS. Full article
(This article belongs to the Special Issue Applied Audio Interaction)
Show Figures

Figure 1

Figure 1
<p>Overview of VSS construction utilizing the proposed method.</p>
Full article ">Figure 2
<p>Comparison of a real sound source and a focused VSS constructed by WFS.</p>
Full article ">Figure 3
<p>Block diagram of the crossfade filters in the proposed method.</p>
Full article ">Figure 4
<p>Experimental arrangement of the evaluation experiments.</p>
Full article ">Figure 5
<p>Loudspeaker array used in the experiments.</p>
Full article ">Figure 6
<p>Results concerning sound pressure transition along <span class="html-italic">y</span>-axis.</p>
Full article ">Figure 7
<p>Results regarding sound pressure distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 1.0).</p>
Full article ">Figure 8
<p>Results for sound pressure distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 2.0).</p>
Full article ">Figure 9
<p>Results on LSD distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 1.0).</p>
Full article ">Figure 10
<p>Results on LSD distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 2.0).</p>
Full article ">Figure 11
<p>Results on direct-to-reverberant ratio (DRR) transition along <span class="html-italic">y</span>-axis.</p>
Full article ">Figure 12
<p>Results on DRR distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 1.0).</p>
Full article ">Figure 13
<p>Results on DRR distribution for <math display="inline"><semantics> <msub> <mi mathvariant="bold-italic">r</mi> <mi mathvariant="normal">S</mi> </msub> </semantics></math> = (0.0, 2.0).</p>
Full article ">Figure 14
<p>Results on subjective distance perception.</p>
Full article ">
22 pages, 1314 KiB  
Article
Area and Performance Estimates of Finite State Machines in Reconfigurable Systems
by Valery Salauyou
Appl. Sci. 2024, 14(24), 11833; https://doi.org/10.3390/app142411833 - 18 Dec 2024
Viewed by 378
Abstract
Modern reconfigurable systems are typically implemented in field-programmable gate arrays (FPGAs) based on look-up tables (LUTs). Finite state machines (FSMs) perform the functions of control devices and are integral to reconfigurable systems. When designing reconfigurable systems, the problem of optimizing the area and [...] Read more.
Modern reconfigurable systems are typically implemented in field-programmable gate arrays (FPGAs) based on look-up tables (LUTs). Finite state machines (FSMs) perform the functions of control devices and are integral to reconfigurable systems. When designing reconfigurable systems, the problem of optimizing the area and performance of FSMs often arises. The FSM synthesis and state encoding methods generally use only one estimate of the FSM area or performance. However, regardless of the computational complexity of the FSM synthesis or state encoding method, if the estimate incorrectly reflects the optimization aim, the result is far from the optimal solution. This paper proposes several estimates of the area and performance of FSMs implemented in LUT-based FPGAs. The effectiveness of the proposed estimates was investigated using the sequential method for FSM state encoding. Experimental studies on benchmarks showed that the FSM area decreases on average from 3.8% to 6.5%, compared to known approaches (for some cases by 33.3%), while the performance increases on average from 3.5% to 7.3% (for some cases by 27.6%). Recommendations for the practical use of the proposed estimates are also provided. The Conclusions section highlights promising directions for future research. Full article
Show Figures

Figure 1

Figure 1
<p>Generalized structural model of an FSM.</p>
Full article ">Figure 2
<p>Generalized decomposition structures: (<b>a</b>) sequential; (<b>b</b>) parallel.</p>
Full article ">Figure 3
<p>Efficiency by area of the estimates considered: <span class="html-italic">Average</span> is the place in order by average value area; <span class="html-italic">Best</span> is the number of best solutions; <span class="html-italic">Unique</span> is the number of unique solutions.</p>
Full article ">Figure 4
<p>Efficiency by performance of the estimates considered: <span class="html-italic">Average</span> is the place in order by average value performance; <span class="html-italic">Best</span> is the number of best solutions; <span class="html-italic">Unique</span> is the number of unique solutions.</p>
Full article ">
14 pages, 3259 KiB  
Communication
Parallel DNA Synthesis to Produce Multi-Usage Two-Dimensional Barcodes
by Etkin Parlar and Jory Lietard
Appl. Sci. 2024, 14(24), 11663; https://doi.org/10.3390/app142411663 - 13 Dec 2024
Viewed by 549
Abstract
Data storage on DNA has emerged as a molecular approach to safeguarding digital information. Microarrays are an excellent source of complex DNA sequence libraries and are playing a central role in the development of this technology. However, the amount of DNA recovered from [...] Read more.
Data storage on DNA has emerged as a molecular approach to safeguarding digital information. Microarrays are an excellent source of complex DNA sequence libraries and are playing a central role in the development of this technology. However, the amount of DNA recovered from microarrays is often too small, and a PCR amplification step is usually required. Primer information can be conveyed alongside the DNA library itself in the form of readable barcodes made of DNA on the array surface. Here, we present a synthetic method to pattern QR and data matrix barcodes using DNA photolithography, phosphoramidite chemistry and fluorescent labeling. Patterning and DNA library synthesis occur simultaneously and on the same surface. We manipulate the chemical composition of the barcodes to make them indelible, erasable or hidden, and a simple chemical treatment under basic conditions can reveal or degrade the pattern. In doing so, information crucial to retrieval and amplification can be made available by the user at the appropriate stage. The code and its data contained within are intimately linked to the library as they are synthesized simultaneously and on the same surface. This process is, in principle, applicable to any in situ microarray synthesis method, for instance, inkjet or electrochemical DNA synthesis. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>A</b>) Microarray subdivision of the addressable area into areas for library synthesis and for barcode synthesis. The barcode area is a strip of ~150 × 768 pixels, or ~2.1 × 10.7 mm<sup>2</sup> given the size of a single addressable unit (14 × 14 μm<sup>2</sup>), and contains up to four DNA barcodes (QR codes or data matrix). (<b>B</b>) The DNA library synthesized in the library area is a 97mer with both forward and reverse primers (in italic) synthesized along with the insert. A Cy3 dye terminates the strand at the 5′ end. (<b>C</b>) An example of a minimal, digitally created QR code delivering primer sequence information upon scanning and thus allowing for the amplification of the synthesized DNA.</p>
Full article ">Figure 2
<p>Photolithographic process of barcoded microarray synthesis. (<b>A</b>) Two separate lists of DNA sequences are used to populate the two specified areas of microarray synthesis, one for the DNA pool and one for the barcode strip. The DNA sequences and their Cartesian coordinates serve to create a series of instructions for parallel DNA synthesis using photolithography, yielding a fluorescently labeled DNA microarray. (<b>B</b>) Toolbox of phosphoramidites employed in the synthesis of barcoded DNA arrays: standard photoprotected (benzyl-nitrophenylpropyloxycarbonyl, Bz-NPPOC) DNA phosphoramidites (top) and base-cleavable succinyl-dT and Cy3 phosphoramidites (bottom).</p>
Full article ">Figure 3
<p>Chemical design of the “persist”, “appear” and “fade” QR codes. (<b>A</b>) Expected behavior of the three barcode types after synthesis (top) and after DNA deprotection (bottom). (<b>B</b>) The outcome of the EDA treatment, besides the removal of all protecting groups, was the hydrolysis of the ester functionality, which released all cleavable DNA from the surface. This allowed for the library to be retrieved as well as for fluorescence to massively decrease on all cleavable spots. (<b>C</b>) Schematic representation of the chemical composition of black and white pixels for all three QR types. The hollow black square represents the cleavable dT unit, and the tag is the fluorescent Cy3 marker.</p>
Full article ">Figure 4
<p>Scanned fluorescent DNA QR codes before (<b>A</b>) and after (<b>B</b>) EDA treatment. The EDA step removes the protecting groups on DNA and cleaves the oligonucleotides wherever a succinyl-dT was inserted. The “persist” code only contains non-cleavable DNA, the “appear” code contains cleavable DNA in the black pixels of the QR code and the “fade” code is cleavable at the labeled pixels only. Scanning was performed in a microarray scanner at a 532 nm excitation wavelength and 2.5 μm resolution. The scale bar is ~100 μm.</p>
Full article ">Figure 5
<p>Fading barcode visibility after an initial cleavage in EDA for 2 h and under increased brightness and contrast settings (left). Further treatment in EDA to induce additional cleavage in the labeled areas (16 h, then 72 h total) leads to minimal additional cleavage but retains the barcoding pattern. Signal/noise is understood as the ratio between fluorescence in the labeled areas (white pixels of the QR image) and background fluorescence in the non-labeled black pixels. Signal range refers to the range of Cy3 fluorescence in the labeled areas, in arbitrary units. Scale bar is ~100 μm.</p>
Full article ">Figure 6
<p>Design concept of the improved fading QR code. Three new strategies are investigated, and the corresponding DNA QR codes are synthesized next to each other on the same microarray. The single cut approach includes a single succinyl-dT unit on both black and white pixels; the mixed-cut approach contains multiple cleavage sites in the DNA (squared dTs in the sequence) at the level of the white pixels; and the multi-cuts approach replaces all dTs with succinyl-dT on both white and black pixels. The green tag corresponds to a 5′-Cy3 fluorescent marker.</p>
Full article ">Figure 7
<p>Fluorescence scans of the barcode strip of a DNA microarray made with the second design for fading QR codes. The array was scanned on a microarray scanner, GenePix 4100A, at a 5 μm resolution with 532 nm wavelength excitation. (<b>A</b>) Scan post-synthesis and pre-treatment with EDA. (<b>B</b>) Scan post-treatment with EDA for 2 h and under similar brightness and contrast settings as for the pre-treatment scan. (<b>C</b>) EDA-treated array and its corresponding scan under high brightness levels. (<b>D</b>) Extreme brightness and contrast adjustments in a graphics editor are necessary to partially reveal a pattern of labeled/non-labeled features in the multi-cut design, with the barcode being largely non-functional.</p>
Full article ">
22 pages, 5132 KiB  
Article
Zn-Layered Double Hydroxide Intercalated with Graphene Oxide for Methylene Blue Photodegradation and Acid Red Adsorption Studies
by Rahmah H. Al-Ammari, Salwa D. Al-Malwi, Mohamed A. Abdel-Fadeel, Salem M. Bawaked and Mohamed Mokhtar M. Mostafa
Catalysts 2024, 14(12), 897; https://doi.org/10.3390/catal14120897 - 6 Dec 2024
Viewed by 992
Abstract
This study focuses on the synthesis of a novel layered double hydroxide and its application in two environmental remediation processes. Graphene oxide, a two-dimensional material, has potential applications in this field. However, its tendency to agglomerate restricts its usability. Our objective was to [...] Read more.
This study focuses on the synthesis of a novel layered double hydroxide and its application in two environmental remediation processes. Graphene oxide, a two-dimensional material, has potential applications in this field. However, its tendency to agglomerate restricts its usability. Our objective was to increase the morphology and performance of layered double hydroxide (LDH) by combining GO with hydrotalcite. The LDH/GO nanohybrids were utilized as photocatalysts for the degradation of methylene blue (MB) dye and were investigated as sorbents for acid red (A.R) dye in water. In order to achieve this objective, ZnAl-NO3 LDH was synthesized using the co-precipitation method, with a Zn:Al ratio of ~3. Subsequently, the LDH was intercalated with varying ratios of as-received graphene oxide. An array of analytical techniques, including X-ray diffraction (XRD), Fourier transform infrared spectroscopy (FT-IR), X-ray photoelectron spectroscopy (XPS) measurements, N2 physisorption, scanning electron microscopy–energy-dispersive X-ray analysis (SEM-EDX), and diffuse reflectance UV–vis spectra (DR UV-vis), were employed to examine the physicochemical properties of the synthesized LDH. These techniques confirmed that the obtained material is zinc-aluminum hydrotalcite intercalated with GO. The addition of graphene oxide (GO) to the layered double hydroxide (LDH) structure improved the performance of the hydrotalcite. As a result, the composite ZnAl-LDH-10 shows significant potential in the field of photocatalytic degradation of MB. Additionally, the incorporation of GO enhanced the absorption of light in the visible region of the spectra, leading to improved elimination of A.R compared to LDH without GO or other ratios of GO. Full article
(This article belongs to the Special Issue Green Chemistry and Catalysis)
Show Figures

Figure 1

Figure 1
<p>XRD of synthesized pure ZnAl-LDH (◆), ZnAl-LDH/GO nanocomposites, and GO (<b>*</b>).</p>
Full article ">Figure 2
<p>(<b>a</b>) XPS survey spectra. (<b>b</b>–<b>e</b>) Deconvoluted XPS spectra of synthesized pure ZnAl-LDH, ZnAl-LDH/GO nanocomposites, and GO.</p>
Full article ">Figure 3
<p>(<b>a</b>) UV-vis diffuse reflectance spectra. (<b>b</b>) Energy band gaps of synthesized pure ZnAl-LDH and ZnAl-LDH/GO nanocomposites.</p>
Full article ">Figure 4
<p>Comparative studies of photocatalytic efficiency of the various catalysts under UV light.</p>
Full article ">Figure 5
<p>The effects of different parameters on photodegradation of MB under UV light: (<b>a</b>) pH of solution, (<b>b</b>) dye concentration, (<b>c</b>) mass of catalysts, and (<b>d</b>) elevated values of the linear regression coefficients (R<sup>2</sup>).</p>
Full article ">Figure 6
<p>Photocatalytic cycles of ZnAl-LDH-10 nanocomposite at pH 10 under UV light.</p>
Full article ">Figure 7
<p>Effect of different parameters on the percentage of adsorption of A.R dye on pure and modified ZnAl-LDH solid phase: (<b>A</b>) pH, (<b>B</b>) adsorbent mass, (<b>C</b>) shaking time, (<b>D</b>) and temperature.</p>
Full article ">Figure 7 Cont.
<p>Effect of different parameters on the percentage of adsorption of A.R dye on pure and modified ZnAl-LDH solid phase: (<b>A</b>) pH, (<b>B</b>) adsorbent mass, (<b>C</b>) shaking time, (<b>D</b>) and temperature.</p>
Full article ">Figure 8
<p>Curves of different kinetic models for uptake of A.R dye in pure and modified ZnAl-LDH vs. time: (<b>A</b>) Weber–Morris, (<b>B</b>) fractional power, (<b>C</b>) Lagergren pseudo-first order, (<b>D</b>) pseudo-second-order, and (<b>E</b>) Elovich models. The experimental conditions are detailed in the batch extraction stage.</p>
Full article ">Figure 9
<p>Curves of ln Kc against 1000/T for uptake of A.R dye from aquatic solution by synthesized pure ZnAl-LDH and ZnAl-LDH/GO nanocomposites.</p>
Full article ">Figure 10
<p>The efficiency of A.R dye removal by synthesized pure ZnAl-LDH and ZnAl-LDH-10 from real three samples (experimental conditions: 25 mL solution, contact time = 120 min, pH solution = 2, temperature = 308 K, 15 mg of solid phase, and 20 mg L<sup>−1</sup> concentration of A.R dye).</p>
Full article ">Scheme 1
<p>The photocatalytic degradation mechanism of modified ZnAl-LDH nanocomposites ((<b>a</b>): band gap calculated for pure ZnAl-LDH before the intercalation with GO, (<b>b</b>): band gap calculated after intercalation of ZnAl-LDH with GO, (<b>c</b>): photolytic degradation of MB dye using the ZnAl-LDH/GO nanocomposite).</p>
Full article ">
13 pages, 3632 KiB  
Article
Lethal and Sublethal Toxicity of Nanosilver and Carbon Nanotube Composites to Hydra vulgaris—A Toxicogenomic Approach
by Joelle Auclair, Eva Roubeau-Dumont and François Gagné
Nanomaterials 2024, 14(23), 1955; https://doi.org/10.3390/nano14231955 - 5 Dec 2024
Viewed by 721
Abstract
The increasing use of nanocomposites has raised concerns about the potential environmental impacts, which are less understood than those observed with individual nanomaterials. The purpose of this study was to investigate the toxicity of nanosilver carbon-walled nanotube (AgNP–CWNT) composites in Hydra vulgaris. [...] Read more.
The increasing use of nanocomposites has raised concerns about the potential environmental impacts, which are less understood than those observed with individual nanomaterials. The purpose of this study was to investigate the toxicity of nanosilver carbon-walled nanotube (AgNP–CWNT) composites in Hydra vulgaris. The lethal and sublethal toxicity was determined based on the characteristic morphological changes (retraction/loss of tentacles and body disintegration) for this organism. In addition, a gene expression array was optimized for gene expression analysis for oxidative stress (superoxide dismutase, catalase), regeneration and growth (serum response factor), protein synthesis, oxidized DNA repair, neural activity (dopamine decarboxylase), and the proteasome/autophagy pathways. The hydras were exposed for 96 h to increasing concentrations of single AgNPs, CWNTs, and to 10% AgNPs–90% CWNTs, and 50% AgNPs–50% CNWT composites. Transmission electron microscopy (TEM) and energy dispersive X-ray spectroscopy (EDS) analysis revealed the presence of AgNPs attached to the carbon nanotubes and AgNP aggregates. The data revealed that the AgNP–CWNT composites were more toxic than their counterparts (AgNPs and CNWT). The sublethal morphological changes (EC50) were strongly associated with oxidative stress and protein synthesis while lethal morphological changes (LC50) encompassed changes in dopamine activity, regeneration, and proteasome/autophagic pathways. In conclusion, the toxicity of AgNP–CWNT composites presents a different pattern in gene expression, and at lower threshold concentrations than those obtained for AgNPs or CWNTs alone. Full article
(This article belongs to the Special Issue Advances in Toxicity of Nanoparticles in Organisms (2nd Edition))
Show Figures

Figure 1

Figure 1
<p>Gene expression changes in hydra exposed to various forms of silver. Hydra were exposed to carbon-walled nanotubes (CWNTs), AgNPs, 10% AgNPs–90% CWNT, and 50% AgNPs–CWNT composites. The data is expressed as the median (star symbol), the 25th–75th quantiles (box), and the data range (minimum–maximum, brackets).</p>
Full article ">Figure 1 Cont.
<p>Gene expression changes in hydra exposed to various forms of silver. Hydra were exposed to carbon-walled nanotubes (CWNTs), AgNPs, 10% AgNPs–90% CWNT, and 50% AgNPs–CWNT composites. The data is expressed as the median (star symbol), the 25th–75th quantiles (box), and the data range (minimum–maximum, brackets).</p>
Full article ">Figure 2
<p>Hierarchical tree analysis of CNT, various forms of silver, and toxicity. The analysis was performed on the toxicity thresholds for gene expression changes (<a href="#nanomaterials-14-01955-t002" class="html-table">Table 2</a>). The distance was calculated based on (1 − R) on the x axis.</p>
Full article ">Figure 3
<p>Discriminant function analysis of gene expression. Discriminant function analysis was performed on the gene expression data at the same concentration range (3–6 ug/L. The points represent the mean distribution of the scored data and the most significant gene changes are found in the parenthesis for each factor (axis).</p>
Full article ">
19 pages, 3016 KiB  
Article
Phase-Only Transmit Beampattern Synthesis Method for Cluttered Environments for Airborne Radar
by Jing Shi, Cao Zeng, Lichu Lai and Jiaqi Zhang
Electronics 2024, 13(23), 4766; https://doi.org/10.3390/electronics13234766 - 2 Dec 2024
Viewed by 419
Abstract
In order to solve the problem of strong downward clutter jamming in airborne radar detection, we propose a phase-only transmit beampattern synthesis method. Firstly, with the aim of minimizing the sidelobe gain in the cluttered region, the desired radiation pattern is constructed by [...] Read more.
In order to solve the problem of strong downward clutter jamming in airborne radar detection, we propose a phase-only transmit beampattern synthesis method. Firstly, with the aim of minimizing the sidelobe gain in the cluttered region, the desired radiation pattern is constructed by using terrain environmental information from where the airborne radar operates. Secondly, an optimization model for phase-only transmit beampattern synthesis accounting for four constraints (the mainlobe gain, the sidelobe gain in the highly cluttered region, the sidelobe gain at other angles, and the amplitude of the weight vector) is established. The Alternating Direction Method of Multipliers (ADMM) is then used to find the iterative solution. Based on the results of four sets of simulation examples designed to verify the effectiveness of the proposed method, it is concluded that the method can reduce the echo intensity in the cluttered region and is suitable for a wide range of array configurations. Full article
(This article belongs to the Special Issue Advances in Array Signal Processing for Diverse Applications)
Show Figures

Figure 1

Figure 1
<p>The program flow of the proposed beampattern synthesis method.</p>
Full article ">Figure 2
<p>The relationship between clutter echo power and <math display="inline"><semantics> <mi>θ</mi> </semantics></math> simulated by using the Morchin model: (<b>a</b>) ground clutter; (<b>b</b>) sea clutter.</p>
Full article ">Figure 3
<p>Simulation results of Example 1: (<b>a</b>) evolution curve; (<b>b</b>) amplitude- and phase-weighted results; (<b>c</b>) beampattern synthesis results; (<b>d</b>) unnormalized beampattern synthesis results; (<b>e</b>) echo signal power.</p>
Full article ">Figure 4
<p>Simulation results of Example 2: (<b>a</b>) evolution curve; (<b>b</b>) amplitude- and phase-weighted results; (<b>c</b>) beampattern synthesis results; (<b>d</b>) unnormalized beampattern synthesis results; (<b>e</b>) echo signal power.</p>
Full article ">Figure 5
<p>Simulation results of Example 3: (<b>a</b>) array position; (<b>b</b>) evolution curve; (<b>c</b>) amplitude- and phase-weighted results; (<b>d</b>) beampattern synthesis results; (<b>e</b>) unnormalized beampattern synthesis results; (<b>f</b>) 3D representations of synthesized beampattern; (<b>g</b>) standard beampattern; (<b>h</b>) unnormalized standard beampattern; (<b>i</b>) 3D representations of standard beampattern; (<b>j</b>) echo signal power of gain-free beampattern; (<b>k</b>) echo signal power of original beampattern; (<b>l</b>) echo signal power of proposed algorithm.</p>
Full article ">Figure 6
<p>Simulation results of Example 4: (<b>a</b>) array position; (<b>b</b>) evolution curve; (<b>c</b>) amplitude- and phase-weighted results; (<b>d</b>) beampattern synthesis results; (<b>e</b>) unnormalized beampattern synthesis results; (<b>f</b>) 3D representations of synthesized beampattern; (<b>g</b>) standard beampattern; (<b>h</b>) unnormalized standard beampattern; (<b>i</b>) 3D representations of standard beampattern; (<b>j</b>) echo signal power of gain-free beampattern; (<b>k</b>) echo signal power of original beampattern; (<b>l</b>) echo signal power of proposed algorithm.</p>
Full article ">Figure 6 Cont.
<p>Simulation results of Example 4: (<b>a</b>) array position; (<b>b</b>) evolution curve; (<b>c</b>) amplitude- and phase-weighted results; (<b>d</b>) beampattern synthesis results; (<b>e</b>) unnormalized beampattern synthesis results; (<b>f</b>) 3D representations of synthesized beampattern; (<b>g</b>) standard beampattern; (<b>h</b>) unnormalized standard beampattern; (<b>i</b>) 3D representations of standard beampattern; (<b>j</b>) echo signal power of gain-free beampattern; (<b>k</b>) echo signal power of original beampattern; (<b>l</b>) echo signal power of proposed algorithm.</p>
Full article ">
Back to TopTop