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20 pages, 6726 KiB  
Article
Rapid and Facile Organic Ion-Associate Liquid-Phase Extraction and Spectrophotometric Quantification of Nitrite in Environmental Water Samples
by Noriko Hata, Kazuki Minoshima, Kei Ito, Nozomi Kohama, Kazuto Sazawa, Sachiko Osada, Takuya Okazaki, Shigeru Taguchi and Hideki Kuramitz
Molecules 2025, 30(5), 1044; https://doi.org/10.3390/molecules30051044 - 25 Feb 2025
Viewed by 202
Abstract
Nitrite is a health and environmental hazard and pollutes water sources globally, but sensitive, rapid, and facile quantification methods are lacking. Herein, we report a method for extracting and quantifying low-concentration nitrite in surface water using minimal sample and solvent volumes. The nitrite [...] Read more.
Nitrite is a health and environmental hazard and pollutes water sources globally, but sensitive, rapid, and facile quantification methods are lacking. Herein, we report a method for extracting and quantifying low-concentration nitrite in surface water using minimal sample and solvent volumes. The nitrite reacted with sulfanilamide and N-1-naphthylethylenediammonium dichloride (NED), yielding an azo dye for extraction into an organic ion-associate liquid phase (IALP) formed in situ using ethylhexyloxypropylammonium and dodecyl sulfate ions. The addition of sodium acetate increased the pH, decreasing the cation charge from +2 to +1, improving extraction efficiency. Further, adding NaCl doubled the IALP volume, reduced the required standing time, and minimally affected absorbance, and adding concentrated HCl to the IALP enhanced the absorbance intensity via dye protonation. Crucially, the method achieved a 30-fold concentration factor compared to traditional pre-treatment methods, even without centrifugation, as well as a limit of detection of 0.09 µg NO2-N/L. Spiked recovery tests with river and seawater samples (93–103%) matched those of established methods. Digital imaging of IALP-extracted lake water yielded a limit of detection of 0.4 µg NO2-N/L. The method is a sensitive, efficient approach for nitrite detection, enabling rapid environmental monitoring via spectrophotometry and digital imaging. Full article
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Graphical abstract

Graphical abstract
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<p>Reactions involved in IALP extraction of azo dyes formed from nitrite. HSA<sup>+</sup>: the cation form of SA.</p>
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<p>Effect of NaOAc addition on the extraction efficiency of azo dyes. The horizontal axis represents the pH of the aqueous phase during extraction, and the vertical axis represents the extraction efficiency of the azo dye into the IALP (<span class="html-italic">A<sub>max</sub></span> = 1). [Nitrite] = 6 µg NO<sub>2</sub>-N/L.</p>
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<p>Relationship between pH and recovery (log {R/(1 − R)}).</p>
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<p>Effect of NaCl concentration on IALP volume. The horizontal axis shows NaCl concentration, and the vertical axis shows the IALP volume 15 min after the addition of the IA reagent.</p>
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<p>Relationship between standing time and IALP volume. The horizontal axis shows the settling time after the addition of the ion-associate-forming reagent, and the vertical axis shows the IALP volume in 50 mL flask.</p>
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<p>Effect of NaCl concentration on absorbance at 540 nm.</p>
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<p>Effect of NaCl concentration on Cl<sup>−</sup> content in the IALP.</p>
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<p>Relationship between EHOPA<sup>+</sup> and DS<sup>−</sup> concentrations and absorbance.</p>
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<p>Relationship between EHOPA<sup>+</sup> and DS<sup>−</sup> concentrations and IALP volume in 100 mL flask.</p>
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<p>Relationship between EHOPA<sup>+</sup> and DS<sup>−</sup> concentrations and log <span class="html-italic">D</span> of (<b>a</b>) NED and (<b>b</b>) SA in the IALP.</p>
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<p>Effect of EHOPA<sup>+</sup> and DS<sup>−</sup> concentrations on absorbance at 540 nm. Red circles are absorbance at 540 nm; larger circles indicate higher absorbance. Green circles mark the optimal combinations reported previously [<a href="#B34-molecules-30-01044" class="html-bibr">34</a>].</p>
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<p>Relationship between log <span class="html-italic">K<sub>ow</sub></span> (from Ref. [<a href="#B40-molecules-30-01044" class="html-bibr">40</a>]) and log <span class="html-italic">D</span>. Red circles, orange square, pink diamond, and white circles represent [H<sub>2</sub>Azo]<sup>2</sup><sup>+</sup> and [HAzo]<sup>+</sup>, HNED<sup>+</sup>, SA, and previous work, respectively. Log <span class="html-italic">D</span> values for estrogens (E1, E2, and EE2), bisphenol-A, and thymol blue are from Ref. [<a href="#B34-molecules-30-01044" class="html-bibr">34</a>].</p>
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<p>Effect of organic solvent on absorbance at 540 nm.</p>
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<p>Relationship between EtOH volume and absorbance.</p>
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<p>Effect of conc. HCl on (<b>a</b>) absorption spectra and (<b>b</b>) absorbance at 540 nm.</p>
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<p>Spiked recovery tests of Furu River water and Yokata Coast seawater (Toyama City, Toyama Prefecture).</p>
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<p>Calibration curve obtained from digital image analysis for IALP extraction of nitrite ions.</p>
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<p>Application to Sakuragaike Lake water. (<b>a</b>) Photograph used for digital image analysis. (<b>b</b>) Standard addition curve. Blue circles represent standard solutions, and white diamonds represent Sakuragaike Lake water (Nanto City, Toyama Prefecture).</p>
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<p>Schematic of the IALP extraction method.</p>
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14 pages, 2081 KiB  
Article
Theoretical Investigation of Single-Atom Catalysts for Hydrogen Evolution Reaction Based on Two-Dimensional Tetragonal V2C2 and V3C3
by Bo Xue, Qingfeng Zeng, Shuyin Yu and Kehe Su
Materials 2025, 18(5), 931; https://doi.org/10.3390/ma18050931 - 20 Feb 2025
Viewed by 171
Abstract
Developing stable and effective catalysts for the hydrogen evolution reaction (HER) has been a long-standing pursuit. In this work, we propose a series of single-atom catalysts (SACs) by importing transition-metal atoms into the carbon and vanadium vacancies of tetragonal V2C2 [...] Read more.
Developing stable and effective catalysts for the hydrogen evolution reaction (HER) has been a long-standing pursuit. In this work, we propose a series of single-atom catalysts (SACs) by importing transition-metal atoms into the carbon and vanadium vacancies of tetragonal V2C2 and V3C3 slabs, where the transition-metal atoms refer to Ti, V, Cr, Mn, Fe, Co, Ni, and Cu. By means of first-principles computations, the possibility of applying these SACs in HER catalysis was investigated. All the SACs are conductive, which is favorable to charge transfer during HER. The Gibbs free energy change (ΔGH*) during hydrogen adsorption was adopted to assess their catalytic ability. For the V2C2-based SACs with V, Cr, Mn, Fe, Ni, and Cu located at the carbon vacancy, excellent HER catalytic performance was achieved, with a |ΔGH*| smaller than 0.2 eV. Among the V3C3-based SACs, apart from the SAC with Mn located at the carbon vacancy, all the SACs can act as outstanding HER catalysts. According to the ΔGH*, these excellent V2C2- and V3C3-based SACs are comparable to the best-known Pt-based HER catalysts. However, it should be noted that the V2C2 and V3C3 slabs have not been successfully synthesized in the laboratory, leading to a pure investigation without practical application in this work. Full article
(This article belongs to the Special Issue Advances in Multicomponent Catalytic Materials)
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<p>The structures and adsorption sites of (<b>a</b>) TM@(4 × 4)-V<sub>2</sub>C<sub>2</sub>-V<sub>C</sub>, (<b>b</b>) TM@(4 × 4)-V<sub>2</sub>C<sub>2</sub>-V<sub>V</sub>, (<b>c</b>) TM@(4 × 4)-V<sub>2</sub>C<sub>2</sub>-V<sub>surf-C</sub>, and (<b>d</b>) TM@(4 × 4)-V<sub>2</sub>C<sub>2</sub>-V<sub>surf-V</sub>. TM atoms are Ti, V, Cr, Mn, Fe, Co, Ni, and Cu for the C/C<sub>surf</sub> vacancies, while they are Ti, Cr, Mn, Fe, Co, Ni, and Cu for the V/V<sub>surf</sub> vacancies.</p>
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13 pages, 3773 KiB  
Article
Transition-Metal-Doped Nickel–Cobalt Layered Double Hydroxide Catalysts for an Efficient Oxygen Evolution Reaction
by Zhihan Li, Wenjing Yi, Qingqing Pang, Meng Zhang and Zhongyi Liu
Materials 2025, 18(4), 877; https://doi.org/10.3390/ma18040877 - 17 Feb 2025
Viewed by 457
Abstract
Hydrogen plays a vital role in the global shift toward cleaner energy solutions, with water electrolysis standing out as one of the most promising techniques for generating hydrogen. Despite its potential, the oxygen evolution reaction (OER) involved in this process faces significant challenges, [...] Read more.
Hydrogen plays a vital role in the global shift toward cleaner energy solutions, with water electrolysis standing out as one of the most promising techniques for generating hydrogen. Despite its potential, the oxygen evolution reaction (OER) involved in this process faces significant challenges, including high overpotentials and slow reaction rates, which underscore the need for advanced electrocatalytic materials to enhance efficiency. Noble metal catalysts are effective but expensive, so transition-metal-based electrocatalysts like nickel–cobalt layered double hydroxides (NiCo LDHs) have become promising alternatives. In this research, a series of NiCo LDH catalysts doped with Fe, Mn, Cu, and Zn were effectively produced using a one-step hydrothermal technique. Among the catalysts, the Fe-doped NiCo LDH exhibited OER activity, achieving a lower overpotential (289 mV) at a current density of 50 mA/cm2, which was far better than the 450 mV of the undoped NiCo LDH. The Mn-, Cu-, and Zn-NiCo LDHs also exhibited lower overpotentials of 414 mV, 403 mV, and 357 mV, respectively, at this current density. The Fe-doped NiCo LDH had a 3D layered nanoflower structure, increasing the surface area for reactant adsorption. The electrochemically active surface area (ECSA), as indicated by the double-layer capacitance (Cdl), was larger in the doped samples. The Cdl value of the Fe-doped NiCo LDH was 3.72 mF/cm2, significantly surpassing the 0.82 mF/cm2 of the undoped NiCo LDH. These changes improved charge transfer and optimized reaction kinetics, enhancing the overall OER performance. This study offers significant contributions to the development of efficient electrocatalysts for the OER, advancing the understanding of key design principles for enhanced catalytic performance. Full article
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<p>SEM images of (<b>a</b>,<b>b</b>) NiCo LDH, (<b>c</b>,<b>d</b>) Fe-NiCo LDH, (<b>e</b>,<b>f</b>) Mn-NiCo LDH, (<b>g</b>,<b>h</b>) Cu-NiCo LDH, and (<b>i</b>,<b>j</b>) Zn-NiCo LDH.</p>
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<p>Structural characterization. (<b>a</b>) XRD patterns and (<b>b</b>) O1s of NiCo LDH, NF, Fe-NiCo LDH, Mn-NiCo LDH, Cu-NiCo LDH, and Zn-NiCo LDH. (<b>c</b>) Ni 2p XPS and (<b>d</b>) Co 2p XPS of Fe-NiCo LDH.</p>
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<p>Co 2p XPS of (<b>a</b>) Mn-NiCo LDH, (<b>b</b>) Cu-NiCo LDH, and (<b>c</b>) Zn-NiCo LDH. Ni 2p XPS of (<b>d</b>) Mn-NiCo LDH, (<b>e</b>) Cu-NiCo LDH, and (<b>f</b>) Zn-NiCo LDH.</p>
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<p>(<b>a</b>) Fe 2p XPS of Fe-NiCo LDH. (<b>b</b>) Mn 2p XPS of Mn-NiCo LDH. (<b>c</b>) Cu 2p XPS of Cu-NiCo LDH. (<b>d</b>) Zn 2p XPS of Zn-NiCo LDH.</p>
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<p>(<b>a</b>) LSV curves, (<b>b</b>) <span class="html-italic">η</span> at a current density of 50 mA cm<sup>−2</sup>, (<b>c</b>) Tafel plots, and (<b>d</b>) linear plots of current density (Δj/2) versus scan rate for NiCo LDH, Fe-NiCo LDH, Mn-NiCo LDH, Cu-NiCo LDH, and Zn-NiCo LDH.</p>
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17 pages, 6677 KiB  
Article
A Green Electromagnetic Energy Harvester with Up-Frequency and Unidirectional Rotation for Smart Pavement
by Keliang Mou, Xiaoping Ji, Xiaojuan Li, Haoyu Zhou, Yunrui Wu and Yeyang Fang
Materials 2025, 18(4), 786; https://doi.org/10.3390/ma18040786 - 11 Feb 2025
Viewed by 445
Abstract
Smart pavement is composed of a monitor network, communication network, data center, and energy supply system, and it requires reliable and efficient energy sources to power sensors and devices. The mechanical energy is wasted and dissipated as heat in traditional pavement; this energy [...] Read more.
Smart pavement is composed of a monitor network, communication network, data center, and energy supply system, and it requires reliable and efficient energy sources to power sensors and devices. The mechanical energy is wasted and dissipated as heat in traditional pavement; this energy can be reused to power low-power devices and sensors for smart pavement. Mechanical energy harvesting systems typically perform through electromagnetic, piezoelectric, and triboelectric methods. Among the different methods, electromagnetic harvesters stand out for their higher output power. However, current electromagnetic harvesters face challenges such as bulky designs, low power density, and high input displacement requirements. This study proposed a green electromagnetic harvester (GEH) based on up-frequency and a unidirectional rotation mechanism to harvest mechanical energy from the pavement. A prototype was designed and prepared. The influence of different parameters on the electrical performance of the harvester was studied by using an MTS test instrument and simulation methods. The results demonstrate that increasing the frequency and optimizing the magnetic array significantly enhances electrical output. The open-circuit voltage in the N-S mode is 3.1 times higher than that in the N-N mode. At a frequency of 9 Hz and a displacement of 3.0 mm, the open-circuit voltage of the GEH is 6.73 V, the maximum power output is 171.14 mW, the peak power density is 1277.16 W/m3, and the voltage has almost no decay after 100,000 cycles. Further, the application of the GEH in charging sensors and capacitors was demonstrated, which indicates the potential of a GEH to power sensors for smart roads. Full article
(This article belongs to the Special Issue Advances in Road Materials and Pavement Design)
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<p>The design of the green electromagnetic harvester.</p>
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<p>Schematic diagram of the working principle and energy harvesting of the energy harvester.</p>
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<p>Magnetic field density distribution of different numbers of magnets.</p>
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<p>Performance comparison of two magnet arrays.</p>
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<p>Influence of magnet mass on output voltage.</p>
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<p>The magnetic field strength between coil and magnet under different gaps.</p>
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<p>(<b>a</b>) Loading process of car on GEH; (<b>b</b>) photograph of the GEH on the MTS.</p>
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<p>Open-circuit voltage of the GEH at different displacement and frequency.</p>
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<p>The output voltages of harvesters under different displacement and different frequencies: (<b>a</b>) 2.0 mm; (<b>b</b>) 2.5 mm; (<b>c</b>) 3.0 mm; (<b>d</b>) the voltage curve of the GEH at 3.0 mm displacement.</p>
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<p>Output power of the GEH under different displacement and frequencies: (<b>a</b>) 2.0 mm; (<b>b</b>) 2.5 mm; (<b>c</b>) 3.0 mm. (<b>d</b>) Comparison of output power under different displacement.</p>
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<p>GEH output voltage in fatigue testing. The blue dot indicates 10,000 loads, and the red dashed line indicates the voltage drop trend.</p>
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<p>Energy harvester performance application test: (<b>a</b>) schematic diagram of circuit connections; (<b>b</b>) charging voltage on different capacitances; (<b>c</b>) charging the hygrothermograph.</p>
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<p>Application scenario of GEH on the road.</p>
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17 pages, 2068 KiB  
Article
Requirements and Test Stand Development for ERS Pantographs
by Alexander Prinz, Kil Young Lee, Abhishek Gupta, Dietmar Göhlich and Sangyoung Park
World Electr. Veh. J. 2025, 16(2), 86; https://doi.org/10.3390/wevj16020086 - 8 Feb 2025
Viewed by 370
Abstract
Electric road systems (ERSs) are a promising solution for electrifying heavy-duty freight transport by providing traction and charging power from the power lines installed along the road. Development of ERSs has been accelerated in the last decade, and several pilot projects have been [...] Read more.
Electric road systems (ERSs) are a promising solution for electrifying heavy-duty freight transport by providing traction and charging power from the power lines installed along the road. Development of ERSs has been accelerated in the last decade, and several pilot projects have been successfully implemented, proving the high level of maturity that the technology has achieved. One crucial step that could be initiated before a rollout is the standardization and certification of ERS infrastructure and system components. For instance, pantographs for overhead ERSs face unique challenges, in that the power transfer should be safe and reliable in the presence of dynamic longitudinal and lateral movements of the vehicle. To tackle this problem, we outline the requirements for overhead ERSs and ERS pantograph testing. Among the key requirements are the rising and lowering times, response to lateral maneuvers, such as lane changes, and high electrical current during stillstand. We introduce our developed test stands capable of testing various aspects of an ERS pantograph. The lateral test stand was developed to test basic functionalities and simulate lateral movements. A second test stand was implemented, to test high currents and the subsequent temperature development. Furthermore, a digital test stand used for planning, design, and modeling is introduced. Full article
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<p>System architecture of an overhead electric road system (left truck picture courtesy of Siemens AG [<a href="#B28-wevj-16-00086" class="html-bibr">28</a>]).</p>
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<p>Approach for requirements derivation for ERS pantograph test stand.</p>
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<p>Overview of the two test stands being developed at the Technical University of Berlin. Above: the lateral test stand. Below: the high-current test stand.</p>
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<p>CAD model of the overhead line suspension system of the lateral test stand.</p>
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<p>Constructed lateral test stand with low and closely spaced OCLs (<b>left</b>) and high and widely spaced OCLs (<b>right</b>). The denoted dimensions are the maximum and minimum distances to be tested. (Dimensions are not to scale).</p>
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<p>CAD model of lateral movement concept (<b>left</b>) and complete lateral test stand (<b>right</b>).</p>
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<p>High-current test stand CAD model (<b>left</b>), implementation (<b>middle</b>), and temperature measurement with a thermal camera (<b>right</b>).</p>
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<p>Test bench for calibration of optical and tactile heat meters and sensors.</p>
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<p>Different coupling states of an ERS pantograph and assembly design of a catenary test stand module.</p>
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14 pages, 5253 KiB  
Article
Research on Monitoring Methods for Electrostatic Discharge Pulses in Spacecraft Dielectric Materials
by Hong Yin, Cunhui Li, Chengxuan Zhao, Xiaogang Qin, Xiaojin Lu, Xuan Wen, Liang Shi, Qing Liu, Jun Wang, Hanwu Jia and Shengsheng Yang
Micromachines 2025, 16(2), 180; https://doi.org/10.3390/mi16020180 - 31 Jan 2025
Viewed by 691
Abstract
Space particle radiation induces charging and discharging phenomena in spacecraft dielectric materials, leading to electrostatic discharge (ESD) and electromagnetic pulses (EMP), which pose significant risks to spacecraft electronic systems by causing interference and potential damage. Accurate and timely monitoring of these phenomena, combined [...] Read more.
Space particle radiation induces charging and discharging phenomena in spacecraft dielectric materials, leading to electrostatic discharge (ESD) and electromagnetic pulses (EMP), which pose significant risks to spacecraft electronic systems by causing interference and potential damage. Accurate and timely monitoring of these phenomena, combined with a comprehensive understanding of their underlying mechanisms, is critical for developing effective protection strategies against satellite charging effects. Addressing in-orbit monitoring requirements, this study proposes the design of a compact sleeve monopole antenna. Through simulations, the relationships between the antenna’s design parameters and its voltage standing wave ratio (VSWR) are analyzed alongside its critical performance characteristics, including frequency band, gain, radiation pattern, and matching circuit. The proposed antenna demonstrates operation within a frequency range of (28.73–31.25) MHz (VSWR < 2), with a center frequency of 30 MHz and a relative bandwidth of 8.4%. Performance evaluations and simulation-based experiments reveal that the antenna can measure pulse signals with electric field strengths ranging from (−1000 to −80) V/m and (80 to 1000) V/m, centered at 25.47 MHz. It reliably monitors discharge pulses generated by electron irradiation on spacecraft-grade FR4 (Flame-Retardant 4) dielectric materials, providing technical support for the engineering application of discharge research in space environments. Full article
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<p>Structural and circuit characteristics of the monopole antenna: (<b>a</b>) schematic of the sleeve monopole antenna structure; (<b>b</b>) equivalent receiving circuit diagram of the antenna.</p>
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<p>Basic dimensions and modeling of a sleeve monopole antenna: (<b>a</b>) cross-sectional diagram of the sleeve monopole antenna; (<b>b</b>) 3D model of the sleeve monopole antenna.</p>
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<p>Simulation analysis of impact of frequency and sleeve height (<span class="html-italic">H</span>) variations on antenna VSWR: (<b>a</b>) impact of frequency variation (<span class="html-italic">L</span> = 4 mm, <span class="html-italic">R</span><sub>0</sub> = 2 mm, <span class="html-italic">R</span> = 6 mm, and <span class="html-italic">H</span> = 5 mm); (<b>b</b>) impact of sleeve height (<span class="html-italic">H</span>) variation (<span class="html-italic">L</span> = 3 mm, <span class="html-italic">R</span><sub>0</sub> = 1 mm and <span class="html-italic">R</span><sub>1</sub> = 4.5 mm).</p>
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<p>Simulation analysis of impact of feed point (<span class="html-italic">L</span>) and insulation layer thickness (<span class="html-italic">t</span>) variations on antenna VSWR: (<b>a</b>) impact of feed point height (<span class="html-italic">L</span>) variation (<span class="html-italic">H</span> = 15 mm, <span class="html-italic">R</span><sub>0</sub> = 0.5 mm, <span class="html-italic">R</span><sub>1</sub> = 4.5 mm); (<b>b</b>) impact of insulation layer thickness (<span class="html-italic">t</span>) variations (<span class="html-italic">H</span> = 20 mm, <span class="html-italic">L</span> = 3 mm).</p>
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<p>The curves of antenna VSWR in the case of <span class="html-italic">H</span> = 20 mm and <span class="html-italic">R</span><sub>1</sub> = <span class="html-italic">R</span><sub>0</sub> + 3 mm.</p>
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<p>Radiation patterns of the sleeve monopole antenna: the radiation patterns at 20 MHz, 30 MHz, and 40 MHz are shown, with the solid line representing the H-plane and the dashed line representing the E-plane.</p>
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<p>VSWR of the sleeve monopole antenna under optimal conditions.</p>
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<p>Antenna matching circuit diagram.</p>
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<p>Simulated values of antenna VSWR under different matching circuits.</p>
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<p>System layout for discharge pulse performance testing of the antenna.</p>
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<p>Response test results of the monopole antenna to the standard electric field.</p>
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<p>Schematic diagram of satellite discharge pulse detection simulation experiment.</p>
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<p>Discharge pulse characteristics of FR4 dielectric material for satellites: (<b>a</b>) temporal characteristics of signals; (<b>b</b>) spectral characteristics of signals.</p>
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19 pages, 12894 KiB  
Article
Comparison Between Crystalline and Amorphous Silicon as Anodes for Lithium Ion Batteries: Electrochemical Performance from Practical Cells and Lithiation Behavior from Molecular Dynamics Simulations
by Geonhee Kim, Min-Ji Yang, Sanghun Lee and Jae-Hyun Shim
Materials 2025, 18(3), 515; https://doi.org/10.3390/ma18030515 - 23 Jan 2025
Viewed by 588
Abstract
As a prominent next-generation anode material for high-capacity applications, silicon stands out due to its potential. Crystalline silicon, which offers a higher initial capacity compared to its amorphous counterpart, presents challenges in practical applications due to its poor cycling performance. In this study, [...] Read more.
As a prominent next-generation anode material for high-capacity applications, silicon stands out due to its potential. Crystalline silicon, which offers a higher initial capacity compared to its amorphous counterpart, presents challenges in practical applications due to its poor cycling performance. In this study, we prepared composites of crystalline and amorphous silicon with graphite, assembled pouch-type full cells, and evaluated their suitability for practical use. The material incorporating amorphous silicon demonstrated superior performance at both high and low rates, as well as various temperatures. Additionally, the changes in cell thickness during charge and discharge, i.e., the volume changes in the anode material, are significantly related to cycling performance. We examined the microscopic interactions between silicon and lithium atoms using molecular dynamics simulations. Our observations indicate that lithium migration within amorphous silicon, which has lower activation energy, is much easier than in crystalline silicon. In crystalline silicon, lithium penetration is greatly influenced by the orientation of the crystal planes, resulting in anisotropic volume expansion during lithiation. Full article
(This article belongs to the Section Energy Materials)
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<p>Initial structures for lithiation processes: (<b>a</b>) c-Si (100), (<b>b</b>) c-Si (110), and (<b>c</b>) a-Si nanofilms and (<b>d</b>) c-Si and (<b>e</b>) a-Si nanospheres. Detailed specifications of the systems are listed in <a href="#materials-18-00515-t001" class="html-table">Table 1</a>. (Purple: Lithium, Yellow: Silicon).</p>
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<p>Characterization of materials: (<b>a</b>) XRD patterns of c-Si and a-Si; HRTEM images with a SAED pattern of (<b>b</b>) c-Si and (<b>c</b>) a-Si; (<b>d</b>) XRD patterns of c-SiC and a-SiC; and an SEM image of (<b>e</b>) c-Si and (<b>f</b>) a-Si.</p>
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<p>(<b>a</b>) Charge/discharge profiles at the first cycle. (<b>b</b>) Rate capability of c-SiC and a-SiC at incremental discharge rates from 0.1 C to 1.5 C. The charge rate is 0.1 C.</p>
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<p>Cycling performance of discharge retention at (<b>a</b>) 0.33 C and 25 °C, (<b>b</b>) 1.0 C and 25 °C, (<b>c</b>) 0.33 C and 45 °C, and (<b>d</b>) 1.0 C and 45 °C. The charge rate of all measurements is 0.2 C.</p>
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<p>Voltage and thickness profiles of DLP (double-layer pouch) cells measured during initial 10 cycles: (<b>a</b>) c-SiC and (<b>b</b>) a-SiC.</p>
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<p>Snapshots of lithiation the process of (<b>a</b>) c-Si (100), (<b>b</b>) c-Si (110), and (<b>c</b>) a-Si nanofilms. (Purple: Lithium, Yellow: Silicon).</p>
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<p>Volume change occurred during the lithiation of silicon nanofilms.</p>
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<p>Variation in density profiles during the lithiation process: (<b>a</b>) Si and (<b>b</b>) Li in c-Si (110) nanofilm, (<b>c</b>) Si and (<b>d</b>) Li in a-Si nanofilm.</p>
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<p>Variation in radial distribution functions during lithiation process: (<b>a</b>) Si-Si and (<b>b</b>) Si-Li in c-Si (110) nanofilm, (<b>c</b>) Si-Si and (<b>d</b>) Si-Li in a-Si nanofilm.</p>
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<p>Snapshots of the lithiation process: (<b>a</b>) c-Si and (<b>b</b>) a-Si spherical nanoparticles. The red arrows in the 50 ps snapshot of (<b>a</b>) indicate the (110) planes.</p>
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<p>(<b>a</b>) Variation in stress profile in the z-direction and (<b>b</b>) atomic strain distribution after 500 ps during lithiation of the (110) plane of c-Si. (<b>c</b>) Variation in stress profile in the z-direction and (<b>d</b>) atomic strain distribution after 500 ps during lithiation of a-Si.</p>
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<p>(<b>a</b>) Snapshots of the lithiation process and (<b>b</b>) atomic strain distribution in crystalline-amorphous combined nanofilms. The red dotted line divides the regions: (Left) a-Si, (Right) c-Si (110).</p>
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12 pages, 4096 KiB  
Article
Benzo[1,2-b:6,5-b’]dithiophene-4,5-diamine: A New Fluorescent Probe for the High-Sensitivity and Real-Time Visual Monitoring of Phosgene
by Yingzhen Zhang, Jun Xiao, Ruiying Peng, Xueliang Feng, Haimei Mao, Kunming Liu, Zhenzhong Liu and Chunxin Ma
Sensors 2025, 25(2), 407; https://doi.org/10.3390/s25020407 - 11 Jan 2025
Viewed by 665
Abstract
The detection of highly toxic chemicals such as phosgene is crucial for addressing the severe threats to human health and public safety posed by terrorist attacks and industrial mishaps. However, timely and precise monitoring of phosgene at a low cost remains a significant [...] Read more.
The detection of highly toxic chemicals such as phosgene is crucial for addressing the severe threats to human health and public safety posed by terrorist attacks and industrial mishaps. However, timely and precise monitoring of phosgene at a low cost remains a significant challenge. This work is the first to report a novel fluorescent system based on the Intramolecular Charge Transfer (ICT) effect, which can rapidly detect phosgene in both solution and gas phases with high sensitivity by integrating a benzo[1,2-b:6,5-b’]dithiophene-4,5-diamine (BDTA) probe. Among existing detecting methods, this fluorescent system stands out as it can respond to phosgene within a mere 30 s and has a detection limit as low as 0.16 μM in solution. Furthermore, the sensing mechanism was rigorously validated through high-resolution mass spectrometry (HRMS) and density functional theory (DFT) calculations. As a result, this fluorescent probing system for phosgene can be effectively adapted for real-time, high-sensitivity sensing and used as a test strip for visual monitoring without the need for specific equipment, which will also provide a new strategy for the fluorescent detection of other toxic materials. Full article
(This article belongs to the Collection Collection:Fluorescent Biosensors)
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<p>(<b>a</b>) Fluorescence emission spectra of the sensing system containing BDTA (100 μM), with or without BTC (200 μM) in indicated solvents; (<b>b</b>) the effect of ACN content on the probes under DMSO-ACN (λem = 490 nm, slits: 10/10 nm), rt for 30 s.</p>
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<p>(<b>a</b>) The fluorescence intensity of the system in the presence and absence of BTC in ACN at the indicated time. (<b>b</b>) Fluorescence emission spectra of BDTA in DMSO before and after the addition of BTC at the incubation time of 30 s. The detection concentration is 100 μM for BDTA in DMSO and 200 μM for BTC in ACN (λem = 490 nm, slits: 10/10 nm).</p>
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<p>(<b>a</b>) Fluorescence spectra of BDTA (100 μM) in response to different concentrations of BTC (0–200 μM), inset: photograph of 100 μM of BDTA with 0–200 μM of BTC 365 nm UV light; (<b>b</b>) linear relationship between BDTA and BTC (λem = 490 nm, slits: 10/10 nm).</p>
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<p>BDTA (100 μM) with various interfering substances (200 μM) and with or without BTC fluorescence response (λem = 490 nm, slits: 10/10 nm).</p>
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<p>Fluorescence changes of BDTA test strip without (<b>a</b>) and with (<b>b</b>) 10 mM BTC solution.</p>
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<p>(<b>a</b>) Schematic representation of phosgene detection using test strips. (<b>b</b>) Photos of BDTA (10 mM)-loaded paper strips exposed to various concentrations of phosgene.</p>
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<p>Frontier molecular orbitals of <b>BDTA</b> (<b>a</b>) and <b>BDTA-CO</b> (<b>b</b>) in DMSO by DFT at the B3LYP/6-31G.</p>
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<p>Detection principle of <b>BDTA</b> for phosgene determination.</p>
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13 pages, 1661 KiB  
Article
Encapsulated LyeTx III Peptide: Cytotoxic Agent Isolated from Lycosa erythrognatha Spider Venom
by Daniel Moreira dos Santos, Livia Ramos Santiago, Nayara Araújo dos Santos, Wanderson Romão, Jarbas Magalhães Resende, Maria Elena de Lima, Márcia Helena Borges and Rosy Iara Maciel de Azambuja Ribeiro
Toxins 2025, 17(1), 32; https://doi.org/10.3390/toxins17010032 - 10 Jan 2025
Viewed by 859
Abstract
The discovery of novel cytotoxic drugs is of paramount importance in contemporary medical research, particularly in the search for treatments with fewer side effects and higher specificity. Antimicrobial peptides are an interesting class of molecules for this endeavor. In this context, the LyeTx [...] Read more.
The discovery of novel cytotoxic drugs is of paramount importance in contemporary medical research, particularly in the search for treatments with fewer side effects and higher specificity. Antimicrobial peptides are an interesting class of molecules for this endeavor. In this context, the LyeTx III, a new peptide extracted from the venom of the Lycosa erythrognatha spider, stands out. The peptide exhibits typical antimicrobial traits: a positive net charge and amphipathic α -helix structure in lipid-like environments. Its unique sequence (GKAMKAIAKFLGR-NH2), identified via mass spectrometry and Edman degradation, shows limited similarity to existing peptides. Significantly, when liposome-encapsulated, LyeTx III demonstrates selective activity against tumor cells in culture. Our MTT results showed that the cytotoxicity of the peptide increased against HN13 cells when administered as liposomes, with their viability in HN13 cells alone being 98%, compared to 38% in liposome-encapsulated form. This finding underscores that the LyeTx III peptide may be a good candidate for the development of new drugs against cancer. Its activity when encapsulated is promising, as it can increase its half-life in the body and can also be targeted to specific tumors. Full article
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<p>Purification of LyeTx III from spider venom by HPLC. (<b>A</b>). The supernatant of the centrifuged crude venom was applied to cation exchange HPLC (TSK gel CM-SW column, 4.6 mm × 250 mm, Tosoh), with a linear NaCl gradient up to 1 M. The flow rate was 0.75 mL·min<sup>−1</sup>, and detection was carried out at 214 nm. (<b>B</b>). The fractions were re-purified by reverse-phase HPLC in a C18 Supercosil column (4.6 mm × 250 mm, Supelco) that was equilibrated with 0.1% aqueous trifluoroacetic acid (TFA), followed by a linear gradient of acetonitrile in 0.1% TFA. The flow was 0.75 mL·min<sup>−1</sup>, and detection was carried out at 214 nm. The arrow shows the fraction of peptide LyeTx III.</p>
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<p><span class="html-italic">m</span>/<span class="html-italic">z</span> determined by MALDI-ToF (Autoflex III–Bruker Daltonics) in positive linear mode.</p>
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<p>Calcein release from liposomes provoked by LyeTx III. (<b>A</b>) Rate of calcein leakage was monitored in liposomes composed of L-α-phosphatidylcholine. LyeTx III was introduced to liposome mixture at varying concentrations, two minutes after incubation at 37 °C. (<b>B</b>) Dose–response curve of calcein release induced by LyeTx III in POPC. Fluorescence emission readings were taken four minutes following exposure to toxin.</p>
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<p>Secondary-structure CD spectra of LyeTxIII at different TFE percentages. The experiment was carried out by incubating the peptide at a concentration of 0.1 mg·mL<sup>−1</sup> in 0.02 mM (0.6%) TFE to 20 mM (60%) TFE, scanning the spectrum from 190 to 280 nm and using 4 accumulations in a spectropolarimeter Jasco-715 (Jasco, Tokyo, Japan).</p>
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<p>LyeTx III liposome reduced HN13 cells’ viability. LyeTxIII peptide alone at 45 µM and LyeTxIII peptide at 45 µM, encapsulated in liposome. *, ***, and ****: statistical significance level <span class="html-italic">p</span> &lt; 0.05, <span class="html-italic">p</span> &lt; 0.0005, and <span class="html-italic">p</span> &lt; 0.0001, respectively.</p>
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19 pages, 5506 KiB  
Article
Binder-Less Molybdenum Doped CoO Based Integrated Electrodes Fabricated by Electric Discharge Corrosion for High-Efficiency Supercapacitors
by Ri Chen, Zehan Xu, Yunying Xu, Tujun Lei, Dawei Liu, Chunlong Chen, Wenxia Wang, Igor Zhitomirsky, Muchao Qu and Guoying Zhang
Materials 2025, 18(1), 80; https://doi.org/10.3390/ma18010080 - 27 Dec 2024
Viewed by 3488
Abstract
Due to its low cost, natural abundance, non-toxicity, and high theoretical capacitance, cobalt oxide (CoO) stands as a promising candidate electrode material for supercapacitors. In this study, binder-less molybdenum doped CoO (Mo@CoO) integrated electrodes were one-step fabricated using a simple electric discharge corrosion [...] Read more.
Due to its low cost, natural abundance, non-toxicity, and high theoretical capacitance, cobalt oxide (CoO) stands as a promising candidate electrode material for supercapacitors. In this study, binder-less molybdenum doped CoO (Mo@CoO) integrated electrodes were one-step fabricated using a simple electric discharge corrosion (EDC) method. This EDC method enables the direct synthesis of Mo@CoO active materials with oxygen vacancy on cobalt substrates, without any pre-made templates, conductive additives, or chemicals. Most importantly, the EDC method enables precise control over the discharge processing parameter of pulse width, which facilitates tailoring the surface morphologies of the as-prepared Mo@CoO active materials. It was found that the fabricated Mo@CoO based symmetric supercapacitor prepared by a pulse width of 24 μs (Mo@CoO-SCs24) achieved a maximum areal capacitance 36.0 mF cm−2 (0.15 mA cm−2), which is 1.83 and 1.97 times higher than that of Mo@CoO-SCs12 and Mo@CoO-SCs36. Moreover, the Mo@CoO-SCs24 devices could be worked at 10 V s−1, which demonstrates their fast charge/discharge characteristic. These results demonstrated the significant potential of the EDC strategy for efficiency fabricating various metal oxide binder-less integrated electrodes for various applications, like supercapacitors, batteries and sensors. Full article
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<p>The process of fabricating binder-less Mo@CoO integrated electrodes and Mo@CoO-SCs using EDC technology. (<b>a</b>–<b>c</b>) Fabrication procedures for binder-free Mo@CoO integrated electrodes, and (<b>d</b>–<b>e</b>) assembly process for Mo@CoO-SCs.</p>
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<p>SEM pictures for Mo@CoO integrated electrodes prepared using EDC with different pulse widths: (<b>a</b>) Mo@CoO-12, (<b>b</b>) Mo@CoO-24, and (<b>c</b>) Mo@CoO-36, and their high-resolution counterparts (<b>d</b>) Mo@CoO-12, (<b>e</b>) Mo@CoO-24, and (<b>f</b>) Mo@CoO-36.</p>
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<p>EDS elemental mapping of the Mo@CoO surface for (<b>a</b>) O, (<b>b</b>) Co, and (<b>c</b>) Mo.</p>
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<p>(<b>a</b>)Full XPS spectrum of Mo@CoO electrode, high-resolution XPS spectra of (<b>b</b>) Co 2p (<b>c</b>) Mo 3d, (<b>d</b>) O 1s spectrum of Mo@CoO electrode.</p>
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<p>(<b>a</b>) CV profiles of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 at 20 mV s<sup>−1</sup>, CV profiles of (<b>b</b>) Mo@CoO-SCs12, (<b>c</b>) Mo@CoO-SCs24, and (<b>d</b>) Mo@CoO-SCs36 at various scan rates (5–50 mV s<sup>−1</sup>).</p>
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<p>Corresponding areal capacitance of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 calculated from CV Profiles.</p>
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<p>(<b>a</b>) CV profiles of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 at ultrahigh scan rate of 10 V s<sup>−1</sup>, CV curves for (<b>b</b>) Mo@CoO-SCs12, (<b>c</b>) Mo@CoO-SCs24, and (<b>d</b>) Mo@CoO-SCs36 at various ultrahigh scan rates (1–10 V s<sup>−1</sup>).</p>
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<p>Corresponding areal capacitance of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 calculated from the ultrahigh CV Profiles.</p>
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<p>(<b>a</b>) GCD profiles of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 at 1 mA cm<sup>−2</sup>, (<b>b</b>) corresponding to areal capacitance of Mo@CoO-SCs12, Mo@CoO-SCs24, and Mo@CoO-SCs36 calculated from GCD Profiles at different current densities (0.15–3 mA cm<sup>−2</sup>).</p>
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19 pages, 9987 KiB  
Review
Recent Advances in Ruddlesden–Popper Phase-Layered Perovskite Sr2TiO4 Photocatalysts
by Pei Wang, Lijun Liao, Hongqi Chu, Ying Xie, Zhenzi Li and Wei Zhou
Nanomaterials 2025, 15(1), 20; https://doi.org/10.3390/nano15010020 - 27 Dec 2024
Viewed by 596
Abstract
Sr2TiO4, a prominent member of the Ruddlesden–Popper (RP) perovskite family, has garnered significant interest in photocatalysis, primarily owing to its distinctive two-dimensional (2D) layered structure. In this review, we provide an insightful and concise summary of the intrinsic properties [...] Read more.
Sr2TiO4, a prominent member of the Ruddlesden–Popper (RP) perovskite family, has garnered significant interest in photocatalysis, primarily owing to its distinctive two-dimensional (2D) layered structure. In this review, we provide an insightful and concise summary of the intrinsic properties of Sr2TiO4, focusing on the electronic, optical, and structural characteristics that render it a promising candidate for photocatalytic applications. Moreover, we delve into the innovative strategies that have been developed to optimize the structural attributes of Sr2TiO4. These strategies aim to maximize light absorption, improve charge separation, and accelerate the photocatalytic reaction rates. By highlighting these unique approaches, we strive to contribute to a more profound understanding of the material’s potential and stimulate further advancements in developing Sr2TiO4-based photocatalytic systems. The review not only synthesizes the existing knowledge but also offers a perspective in future directions for research and application. As the field of photocatalysis continues to evolve, Sr2TiO4 stands poised to play a pivotal role in the quest for more efficient and sustainable solar energy conversion technology. Full article
(This article belongs to the Section Energy and Catalysis)
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<p>Publication and citation data on Sr<sub>2</sub>TiO<sub>4</sub> photocatalysis in recent years.</p>
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<p>Schematic diagram of the main content of this review.</p>
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<p>Refined crystal structures and unit-cells of Sr<sub>2</sub>TiO<sub>4</sub>. The dashed rectangles in the crystal structure represent the a × c facet of the corresponding unit cells [<a href="#B27-nanomaterials-15-00020" class="html-bibr">27</a>].</p>
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<p>(<b>a</b>) Ruddlesden–Popper phase of layered oxide, (<b>b</b>) the overview of catalyst surface modification and (<b>c</b>) XRD patterns of Sr<sub>2</sub>TiO<sub>4</sub>, H-Sr<sub>2</sub>TiO<sub>4</sub> and exfoliation of Sr<sub>2</sub>TiO<sub>4</sub> catalysts [<a href="#B45-nanomaterials-15-00020" class="html-bibr">45</a>].</p>
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<p>Photocatalytic CO<sub>2</sub> reduction with H<sub>2</sub>O on catalysts. (<b>a</b>) yield of CH<sub>4</sub>, (<b>b</b>) yield of H<sub>2</sub> (<b>c</b>) yield of C<sub>2</sub>H<sub>6</sub> (<b>d</b>) yield of C<sub>2</sub>H<sub>4</sub>, and (<b>e</b>) yield of CO [<a href="#B45-nanomaterials-15-00020" class="html-bibr">45</a>].</p>
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<p>SEM images of sample No. (<b>a</b>) 1 (<b>b</b>) 2 (<b>c</b>) 3 (<b>d</b>) 4 (<b>e</b>) 5 (<b>f</b>) 6 [<a href="#B25-nanomaterials-15-00020" class="html-bibr">25</a>].</p>
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<p>Degradation diagrams of (<b>a</b>) methyl orange on presence of different Sr<sub>2</sub>TiO<sub>4</sub> (<b>b</b>) different dyes with sample No. 3 [<a href="#B25-nanomaterials-15-00020" class="html-bibr">25</a>].</p>
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<p>XPS spectra of Sr<sub>2</sub>TiO<sub>4−x</sub>F<sub>x</sub> (x = 0, 0.01, 0.03 and 0.05): (<b>a</b>) Ti 2p, (<b>b</b>) O 1s [<a href="#B51-nanomaterials-15-00020" class="html-bibr">51</a>].</p>
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<p>The H<sub>2</sub> production (<b>a</b>) amounts and (<b>b</b>) rates of solar water splitting on Sr<sub>2</sub>TiO<sub>4-x</sub>F<sub>x</sub> (x = 0, 0.01, 0.03, 0.05, and 0.1) under full-range sunlight illumination (λ ≥ 250 nm) [<a href="#B51-nanomaterials-15-00020" class="html-bibr">51</a>].</p>
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<p>(<b>a</b>) Calculated band structures, the total density of states, and partial density of states of constituent elements of Sr<sub>2</sub>TiO<sub>3</sub>F<sub>2</sub>, and Fermi level is marked by dotted orange line; (<b>b</b>) density contour maps of Sr<sub>2</sub>TiO<sub>3</sub>F<sub>2</sub> at VBM and CBM; (<b>c</b>) crystal structure of Sr<sub>2</sub>TiO<sub>4</sub> and Sr<sub>2</sub>TiO<sub>3</sub>F<sub>2</sub> projected along (100) direction; (<b>d</b>) schematic illustration of a built-in electrical field across the single TiO<sub>6</sub> octahedron layer (upper image) and its impact toward the separation of photogenerated electron–hole pairs (lower image), direction of electric field is indicated by red dotted arrow, red and blue balls refer to photogenerated electrons and holes, respectively (for interpretation of the references to color in this figure legend, the reader is referred to the web version of this article) [<a href="#B62-nanomaterials-15-00020" class="html-bibr">62</a>].</p>
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<p>(<b>a</b>) X-ray diffraction patterns of the as-prepared samples: a SrTiO<sub>3</sub>, b SrTiO<sub>3</sub> (La,Cr), c Sr<sub>2</sub>TiO<sub>4</sub>, d Sr<sub>2</sub>TiO<sub>4</sub> (La,Cr), and e Sr<sub>2</sub>TiO<sub>4</sub>/SrTiO<sub>3</sub> (La,Cr), (<b>b</b>) photocatalytic H<sub>2</sub> production activities of the initially synthesized SrTiO<sub>3</sub> (La,Cr), Sr<sub>2</sub>TiO<sub>4</sub> (La,Cr) and Sr<sub>2</sub>TiO<sub>4</sub>/SrTiO<sub>3</sub> (La,Cr) composite samples ([Cr]/([Ti] + [Cr]) = 0.05, [La]/[Cr] = 1.00, molar ratio). Inset: the time course of H<sub>2</sub> evolution, (<b>c</b>) schematic band structure of La and Cr co-doped Sr<sub>2</sub>TiO<sub>4</sub>/SrTiO<sub>3</sub> and its mechanism for H<sub>2</sub> production under visible light irradiation [<a href="#B64-nanomaterials-15-00020" class="html-bibr">64</a>].</p>
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13 pages, 6810 KiB  
Article
Open-Source Equipment Design for Cost-Effective Redox Flow Battery Research
by Trinh V. Dung, Nguyen T. T. Huyen, Nguyen L. T. Huynh, Nguyen T. Binh, Nguyen T. Dat, Nguyen T. T. Nga, Nguyen T. Lan, Hoang V. Tran, Nguyen T. T. Mai and Chinh D. Huynh
ChemEngineering 2024, 8(6), 120; https://doi.org/10.3390/chemengineering8060120 - 28 Nov 2024
Viewed by 973
Abstract
Redox flow batteries (RFBs), with distinct characteristics that are suited for grid-scale applications, stand at the forefront of potential energy solutions. However, progress in RFB technology is often impeded by their prohibitive cost and the limited availability of essential research and development test [...] Read more.
Redox flow batteries (RFBs), with distinct characteristics that are suited for grid-scale applications, stand at the forefront of potential energy solutions. However, progress in RFB technology is often impeded by their prohibitive cost and the limited availability of essential research and development test cells. Addressing this bottleneck, we present herein an open-source device tailored for RFB laboratory research. Our proposed device significantly lowers the financial barriers to research and enhances the accessibility of vital equipment for RFB studies. Employing innovative fabrication methods such as laser cutting, 3D printing, and CNC machining, a versatile and efficient flow cell has been designed and fabricated. Furthermore, our open laboratory research equipment comprises the Opensens potentiostat, charge/discharge testing devices, peristaltic pumps, and inexpensive rotating electrodes. Every individual element contributes significantly to the establishment of an all-encompassing experimental configuration that is both economical and efficient, thereby facilitating expedited progress in RFB research and development. Full article
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<p>The PCB layout of the power module.</p>
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<p>The Nodered dashboard used to control and monitor the charge/discharge module.</p>
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<p>(<b>a</b>) The setup used for the CV experiments, (<b>b</b>) the experimental setup of the RDE and Opensens used in the experiments, (<b>c</b>) the original design with a one-brush electrode, and (<b>d</b>) the dual-brush electrode.</p>
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<p>Cyclic voltammograms of a Pt electrode in: (<b>a</b>) 1 M of vanadium electrolyte with different concentrations of H<sub>2</sub>SO<sub>4</sub>, (<b>b</b>) 0.6M Ce(CH<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> + 4M MSA + x M H<sub>2</sub>SO<sub>4</sub>.</p>
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<p>Cyclic voltammograms of a Pt electrode in 0.6 M Ce(CH<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> + x M MSA (x = 1, 2, 3, 4, 5).</p>
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<p>(<b>a</b>) Linear sweep voltammetry of 0.6 M Ce(CH<sub>3</sub>SO<sub>3</sub>)<sub>3</sub> + 4M MSA + 0.5 M H<sub>2</sub>SO<sub>4</sub> + 2% mol L-Lysine electrolyte with different rotation speeds at a scan rate of 5 mV/s. (<b>b</b>) Levich plot of limiting current versus the square root of the rotation rate (ω<sup>1/2</sup>). (<b>c</b>) Koutecky–Levich plot at different overpotentials. (<b>d</b>) Tafel plot of the logarithm of kinetically limited current versus overpotential.</p>
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<p>Charge/discharge curves of the V-Ce RFB (current I = 0.05 A, with voltage limits at 2.0–0.6 V).</p>
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<p>Coulombic, voltage, and energy efficiency as a function of the cycle number.</p>
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16 pages, 6756 KiB  
Article
Self-Assembled Gold Nanoparticles as Reusable SERS Substrates for Polyphenolic Compound Detection
by Arina Pavlova, Ksenia Maleeva, Ivan V. Moskalenko, Vadim Belyaev, Mikhail V. Zhukov, Demid Kirilenko, Kirill V. Bogdanov and Evgeny Smirnov
Int. J. Mol. Sci. 2024, 25(23), 12785; https://doi.org/10.3390/ijms252312785 - 28 Nov 2024
Viewed by 1081
Abstract
Natural polyphenolic compounds play a pivotal role in biological processes and exhibit notable antioxidant activity. Among these compounds, chlorogenic acid stands out as one of the most widespread and important polyphenols. The accurate detection of chlorogenic acid is crucial for ensuring the quality [...] Read more.
Natural polyphenolic compounds play a pivotal role in biological processes and exhibit notable antioxidant activity. Among these compounds, chlorogenic acid stands out as one of the most widespread and important polyphenols. The accurate detection of chlorogenic acid is crucial for ensuring the quality and classification of the raw materials used in its extraction, as well as the final products in the food, pharmaceutical, and cosmetics industries that contain this bioactive compound. Raman spectroscopy emerges as a powerful analytical tool, particularly in field applications, due to its versatility and sensitivity, offering both qualitative and quantitative analyses. By using the self-assembly of gold nanoparticles at liquid–liquid interfaces and the developed “aqua-print” process, we propose a facile and inexpensive route to fabricate enhanced substrates for surface-enhanced Raman spectroscopy with high reproducibility. To ensure substrate reliability and accurate molecule detection in SERS experiments, a benchmarking procedure was developed. This process involved the use of non-resonant rhodamine 6G dye in the absence of charge transfer and was applied to all synthesized nanoparticles and fabricated substrates. The latter revealed the highest enhancement factor of 4 × 104 for 72 nm gold nanoparticles among nanoparticle diameters ranging from 14 to 99 nm. Furthermore, the enhanced substrate was implemented in the detection of chlorogenic acid with a concentration range from 10 μM to 350 μM, demonstrating high accuracy (R2 > 99%). Raman mapping was employed to validate the good uniformity of the signal (the standard deviation was below 15%). The findings of this study were also supported by DFT calculations of the theoretical Raman spectra, demonstrating the formation of the chlorogenic acid dimer. The proposed method is strategically important for the development of the class of in-field methods to detect polyphenolic compounds in raw materials such as plants, extracted plant proteins, and polyphenolic compounds. Full article
(This article belongs to the Special Issue Properties and Applications of Nanoparticles and Nanomaterials)
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<p>Characterization of synthesized gold nanoparticles. (<b>A</b>) UV-Vis absorbance spectra, (<b>B</b>) particle size distributions and ζ-potentials, and (<b>C</b>) TEM images of synthesized AuNPs of maximal and minimal diameters. Insets: Bar diagrams of particle size distributions based on TEM image data processing (the red curve is the Gaussian fit). The labeling of the samples should be read as the following: <span class="html-italic">Frens</span> = nanoparticles synthesized by the Frens–Turkevich method using one reductant agent: <span class="html-italic">Na<sub>3</sub>Citr</span> = sodium citrate, <span class="html-italic">KAsc</span> = potassium ascorbate, or <span class="html-italic">HAsc</span> = ascorbic acid; <span class="html-italic">SMG</span> = nanoparticles synthesized by Park’s method.</p>
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<p>Morphological characterization of the fabricated enhanced substrates by SEM (<b>A</b>,<b>D</b>), TEM (<b>B</b>,<b>E</b>), and AFM (<b>C</b>,<b>F</b>). Silicon substrates coated with 14 nm AuNPs (<b>A</b>–<b>C</b>) and 72 nm nanoparticles (<b>D</b>–<b>F</b>).</p>
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<p>Benchmarking the enhanced substrate made of 14 nm AuNPs with the non-resonant reporter molecule R6G at varying concentrations (the grey area marks out the peak used for plotting panel B). (<b>A</b>) Recorded surface-enhanced Raman spectra of R6G. (<b>B</b>) Calibration curve demonstrating the linear dependence of the Raman scattering of R6G at a selected wavenumber of 1360 cm<sup>−1</sup>. (<b>C</b>,<b>D</b>) Mapping of the enhanced substrate at an R6G concentration of 150 μM: (<b>C</b>) peak position map and (<b>D</b>) peak intensity map at 1360 cm<sup>−1</sup>.</p>
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<p>Benchmarking the enhanced substrate made of 72 nm AuNPs with the non-resonant reporter molecule R6G at varying concentrations. (<b>A</b>) Recorded surface-enhanced Raman spectra of R6G (the grey area marks out the peak used for plotting panel B). (<b>B</b>) Calibration curve demonstrating the linear dependence of Raman scattering of R6G at a selected wavenumber of 1360 cm<sup>−1</sup>. (<b>C</b>,<b>D</b>) Mapping of the enhanced substrate at an R6G concentration of 150 μM: (<b>C</b>) peak position map and (<b>D</b>) peak intensity map at 1360 cm<sup>−1</sup>.</p>
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<p>Dependence of the analytical enhancement factor on the diameter of AuNPs synthesized by different methods. A Gaussian curve was used as the trend line.</p>
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<p>Detection of CGA dimer on the enhanced substrate made of 72 nm AuNPs by Raman spectroscopy. (<b>A</b>) Experimental spectra on SERS substrates for different concentrations of CGA dimer (the grey area marks out the peak used for plotting panel C). (<b>B</b>) Comparison of the DFT-calculated Raman spectrum with the experimental one. (<b>C</b>) Calibration curve demonstrating the linear dependence of Raman scattering of the CGA dimer at 1615 cm<sup>−1</sup>. (<b>D</b>,<b>E</b>) Mapping of the enhanced substrate at a CGA concentration of 50 μM: (<b>C</b>) peak position map and (<b>D</b>) peak intensity map at 1615 cm<sup>−1</sup>.</p>
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<p>Schematic of AuNP synthesis and SERS substrate preparation procedure. (<b>A</b>) Synthesis of AuNPs with different methods: Frens–Turkevich with trisodium citrate, ascorbic acid, or potassium ascorbate; seed-mediated growth from smallest seed particle obtained by Ferns–Turkevich method. (<b>B</b>) Enhanced substrate fabrication: (<b>i</b>) self-assembly of AuNPs into nanofilm using liquid–liquid interface (MELLDs), (<b>ii</b>) transfer of nanofilm to solid substrate (silicon) with aqua-print technology. Photos demonstrate visual appearance of MELLD and nanofilm on substrate.</p>
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12 pages, 2879 KiB  
Article
Interaction of Phenanthroline-Containing Copper Complexes with Model Phospholipid Membranes
by Priscilla Freddi, Natalia Alvarez, Gianella Facchin and Antonio J. Costa-Filho
Inorganics 2024, 12(12), 307; https://doi.org/10.3390/inorganics12120307 - 26 Nov 2024
Viewed by 938
Abstract
Medicinal Inorganic Chemistry has provided oncology with metallodrugs for cancer treatment, including several promising candidate drugs. In particular, copper(II) coordination compounds with phenanthroline stand out as potential anticancer agents. In this work, we used Differential Scanning Calorimetry and Electron Spin Resonance to investigate [...] Read more.
Medicinal Inorganic Chemistry has provided oncology with metallodrugs for cancer treatment, including several promising candidate drugs. In particular, copper(II) coordination compounds with phenanthroline stand out as potential anticancer agents. In this work, we used Differential Scanning Calorimetry and Electron Spin Resonance to investigate the interaction of the copper phenanthroline complexes [Cu(phen)]2+ and [Cu(L-dipeptide)(phenanthroline) (L-dipeptide: L-Ala-Gly and L-Ala-Phe)) with model lipid membranes (1,2-dipalmitoyl-sn-glycero-3-phosphocholine, DPPC, and 1,2-dipalmitoyl-sn-glycero-3-phospho-(1′-rac-glycerol) sodium salt, DPPG). Our results showed that the complexes interact with the membrane models, fluidizing them. The [Cu(phen)]2+ presented a different localization than the free ligand phen. The dipeptide modulated the localization of the complex in the membrane and the modifications induced in the physicochemical properties of the lipid vesicles. A stronger interaction with DPPG anionic membranes was observed, which mimic membranes with negatively charged surfaces, as found on several tumor cells. Full article
(This article belongs to the Special Issue Evaluation of the Potential Biological Activity of Metallo-Drugs)
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<p>[Cu(dipeptide)(phen)] complex scheme.</p>
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<p>DSC traces from MLVs of DPPC in the absence and the presence of the complexes. The insets show the zoomed-in regions around the pre-transition at 35 °C and the main phase transition at 41 °C.</p>
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<p>DSC traces from MLVs of DPPG in the absence and the presence of the complexes.</p>
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<p>Temperature variation of h<sub>+1</sub>/h<sub>0</sub> for the spin probe DOPTC in MLVs of DPPC (upper panel) and DPPG (lower panel) in the absence and presence of the complexes. The solid lines are guides for the eyes only.</p>
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<p>Temperature variation A<sub>MAX</sub> for the spin probe 5-PCSL in MLVs of DPPC (upper panel) and DPPG (lower panel) in the absence and presence of the complexes. The solid lines are guides for the eyes only.</p>
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<p>Temperature variation of h<sub>−1</sub>/h<sub>0</sub> for the spin probe 16-PCSL in MLVs of DPPC (upper panel) and DPPG (lower panel) in the absence and presence of the complexes. The solid lines are guides for the eyes only.</p>
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<p>FIMs for (<b>a</b>) phen, (<b>b</b>) [CuCl<sub>2</sub>(phen)], (<b>c</b>) [Cu(Ala-Gly)phen] and (<b>d</b>) Cu(Ala-Phe)phen].</p>
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18 pages, 2702 KiB  
Article
Symmetry Breaking of Electronic Structure upon the π→π* Excitation in Anthranilic Acid Homodimer
by Marcin Andrzejak, Joanna Zams, Jakub Goclon and Przemysław Kolek
Molecules 2024, 29(23), 5562; https://doi.org/10.3390/molecules29235562 - 25 Nov 2024
Viewed by 724
Abstract
The main purpose of this study is to characterize the nature of the low-energy singlet excited states of the anthranilic acid homodimer (AA2) and their changes (symmetry breaking) caused by deformation of the centrosymmetric, ground state structure of AA2 towards [...] Read more.
The main purpose of this study is to characterize the nature of the low-energy singlet excited states of the anthranilic acid homodimer (AA2) and their changes (symmetry breaking) caused by deformation of the centrosymmetric, ground state structure of AA2 towards the geometry of the S1 state. We employ both the correlated ab initio methods (approximate Coupled Clusters Singles and Doubles—CC2 and CASSCF/NEVPT2) as well as the DFT/TDDFT calculations with two exchange–correlation functionals, i.e., B3LYP and CAM-B3LYP. The composition of the wavefunctions is investigated using the one-electron transition density matrix and difference density maps. We demonstrate that in the case of AA2, small asymmetric distortions of geometry bring about unproportionally large changes in the excited state wavefunctions. We further provide comprehensive characterization of the AA2 electronic structure, showing that the excitation is nearly completely localized on one of the monomers, which stands in agreement with the experimental evidence. The excitation increases the π-electronic coupling of the substituents and the aromatic ring, but only in the excited monomer, while the changes in the electronic structure of the unexcited monomer are negligible (after geometry relaxation). The increased electronic density strengthens both intra- and intermolecular hydrogen bonds formed by the carbonyl oxygen atom of the excited monomer, making them significantly stronger than in the ground state. Although the overall pattern of changes remains qualitatively consistent across all methods employed, CC2 predicts more pronounced excitation-induced modifications of the electronic structure compared to the more routinely used TDDFT approach. The most important deficiency of the B3LYP functional in the present context is locating two charge-transfer states at erroneously low energies, in close proximity of the S1 and S2 states. The range-corrected CAM-B3LYP exchange–correlation functional gives a considerably improved description of the CT states at the price of overshot excitation energies. Full article
(This article belongs to the Section Computational and Theoretical Chemistry)
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<p>The only detected rotamer R1 of anthranilic acid (<b>left</b>) and the related rotamer of the dimer: R1:::R1 (<b>right</b>).</p>
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<p>The energies of the lowest excited states of the AA dimer (with respect to the ground state energy of the C<sub>2h</sub> structure) calculated at different levels of theory for a series of geometries, starting from the planar, centrosymmetric structure of the electronic ground state (0% of deformation) and gradually distorted towards the structure corresponding to the S<sub>1</sub> excited state (100% of deformation).</p>
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<p>Compositions of the excited states of the AA homodimer in terms of the diabatic components (see text) based on one-electron TDM analysis calculated at different levels of theory. (1–2) in the description of the CT component means that an electron has been transferred from monomer 1 to monomer 2. For consistency of the notation, the excited states for the ground state geometry (0% if deformation) are also described within the framework of the C<sub>s</sub> symmetry group.</p>
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<p>Electron difference densities calculated using CC2 and one of the variants of TDDFT for the S<sub>0</sub>→S<sub>1</sub> excitation calculated at different degrees of geometry deformation from the centrosymmetric structure of the ground state towards the distorted geometry deformation from the centrosymmetric structure of the ground state towards the distorted geometry of the S<sub>1</sub> state of the AA dimer. Blue color signifies regions with increased electron density; red color signifies regions with decreased electron density.</p>
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<p>Mayer bond orders of AA monomer for the ground state (<b>upper panel</b>) and for the S<sub>1</sub> state (<b>lower panel</b>). Changes in the bond orders due to the electronic excitation are given in parentheses.</p>
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<p>Mayer bond orders of AA dimer for the ground state (<b>upper panel</b>) and for the S<sub>1</sub> state (<b>lower panel</b>). Changes in the bond orders due to the electronic excitation are given in parentheses.</p>
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