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Topological magnetic defects in a strong permanent magnet Nd2Fe14B 强永磁体 Nd2Fe14B 中的拓扑磁性缺陷
Pub Date : 2024-10-09 DOI: 10.1016/j.mtquan.2024.100017
Juyoung Jeong , Yongwoo Lee , Shi-Zeng Lin , Yoon Hee Jeong , Hye Jung Chang , Jeehoon Kim
Skyrmions, highly mobile and manipulable magnetic objects, have garnered significant interest for their potential applications in modern magnetic device technology. However, their formation has been limited to a small number of materials due to the delicate balance of magnetic energies involved. In this study, we report the irreversible formation of skyrmions in Nd2Fe14B, a rare-earth permanent magnet characterized by large magnetic anisotropy. Remarkably, these magnetic topological defects exist over a wide range of temperatures and magnetic fields (295–565 K and 0–0.1 T) due to the high Curie temperature and significant magnetic anisotropy of Nd2Fe14B. Our findings not only unveil a new material where skyrmions can form but also open up possibilities for exploring topological defects in various magnetic systems, including strong hard magnets.
Skyrmions 是一种高度移动和可操控的磁性物体,因其在现代磁性器件技术中的潜在应用而备受关注。然而,由于涉及磁能的微妙平衡,它们的形成仅限于少数材料。在这项研究中,我们报告了在钕2铁14B中不可逆地形成天顶子的情况,钕2铁14B是一种稀土永磁体,具有较大的磁各向异性。值得注意的是,由于 Nd2Fe14B 的居里温度高且磁各向异性显著,这些磁拓扑缺陷存在于很宽的温度和磁场范围内(295-565 K 和 0-0.1 T)。我们的发现不仅揭示了一种可以形成天幕的新材料,而且为探索包括强硬磁体在内的各种磁性系统中的拓扑缺陷提供了可能性。
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引用次数: 0
Synthesis of temperature-sensitive boron, nitrogen and sulphur doped carbon dots and their applications 温度敏感的硼、氮和硫掺杂碳点的合成及其应用
Pub Date : 2024-10-04 DOI: 10.1016/j.mtquan.2024.100018
Pingping Liu , Lu Fu , Gerile Aodeng , Lu Ga , Jun Ai
Boron-Sulfur-Nitrogen doped carbon dots (B, N, S-CDs) were prepared by a simple hydrothermal method using 2-Mercaptopyrimidine (C4H4N2S) and citric acid (C6H8N7•H2O) as raw materials. The B, N, S-CDs showed exceptional fluorescence response to Fe2+, TC. The results of the B, N, S-CDs are very promising for the detection of real water samples. In addition, the B, N, S-CDs had a good temperature response (reversible and recoverable fluorescence in the temperature range of 25–65︒C). The low cytotoxicity and in vitro cellular imaging properties exhibited by this carbon dot also greatly enhance their utility.
以 2-巯基嘧啶(C4H4N2S)和柠檬酸(C6H8N7-H2O)为原料,通过简单的水热法制备了掺硼-硫-氮的碳点(B, N, S-CDs)。B,N,S-CDs 对 Fe2+、TC 显示出特殊的荧光响应。B、N、S-CDs 的结果非常适合实际水样的检测。此外,B、N、S-CDs 还具有良好的温度响应(在 25-65︒C 的温度范围内,荧光可逆且可恢复)。这种碳点表现出的低细胞毒性和体外细胞成像特性也大大提高了其实用性。
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引用次数: 0
Nanometric modulations of the magnetic structure of the element Nd 钕元素磁性结构的纳米调制
Pub Date : 2024-09-23 DOI: 10.1016/j.mtquan.2024.100016
H. Suriya Arachchige , L.M. DeBeer-Schmitt , L.L. Kish , Binod K. Rai , A.F. May , D.S. Parker , G. Pokharel , Wei Tian , Matthew B. Stone , Matthias Frontzek , D.G. Mandrus , M. Bleuel , Z. Islam , G. Fabbris , H.X. Li , S. Gao , H. Miao , S.M. Thomas , P.F.S. Rosa , J.D. Thompson , A.D. Christianson
The rare earth neodymium arguably exhibits the most complex magnetic ordering and series of magnetic phase transitions of the elements. Here we report the results of small-angle neutron scattering (SANS) measurements as a function of temperature and applied magnetic field to study magnetic correlations on nanometer length scales in Nd. We support these results with additional neutron diffraction, thermodynamic and synchrotron x-ray measurements. The SANS measurements reveal the presence of modulation vectors characterizing the ordered spin configuration which exhibit changes in magnitude and direction that are phase dependent. Between 5.9 and 7.6 K an additional modulation vector is observed with magnitude Q = 0.12 Å −1. This scattering appears to originate from order of the Nd layers which contain a center of inversion. Tracking this modulation vector as a function of magnetic field indicates a phase boundary at 1 T. The modulation vectors observed in this study establish the presence of nanometer length scale spin textures which are likely stabilized by frustrated Ruderman–Kittel–Kasuya–Yosida (RKKY) interactions.
稀土钕可以说是磁排序和磁相变系列最复杂的元素。在此,我们报告了小角中子散射(SANS)测量结果与温度和外加磁场的函数关系,以研究钕中纳米长度尺度的磁相关性。我们还通过中子衍射、热力学和同步辐射 X 射线测量来支持这些结果。SANS 测量揭示了有序自旋构型的调制矢量特征,其大小和方向的变化与相位有关。在 5.9 至 7.6 K 之间,还观察到一个额外的调制矢量,其大小为 Q = 0.12 Å-1。这种散射似乎源自包含反转中心的钕层。这项研究中观察到的调制矢量确定了纳米级自旋纹理的存在,这种纹理很可能是通过受挫的 Ruderman-Kittel-Kasuya-Yosida (RKKY) 相互作用而稳定下来的。
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引用次数: 0
Correlated insulators and charge density wave states in chirally twisted triple bilayer graphene 手性扭曲三重双层石墨烯中的相关绝缘体和电荷密度波态
Pub Date : 2024-09-21 DOI: 10.1016/j.mtquan.2024.100015
Geng-Dong Zhou , Yi-Jie Wang , Wen-Xuan Wang , Xiao-Bo Lu , Zhi-Da Song
Motivated by recent experimental observations of displacement-field-tuned correlated insulators at integer and half-integer fillings in chirally twisted triple bilayer graphene (CTTBG) [Phys.Rev.Lett.132.246501], we study the single-particle and interacting physics of CTTBG. We find that there are two inequivalent stacking orders, i.e., AB-AB-BC and AB-AB-AB, and both exhibit flat bands with nontrivial topology. We then use the Hartree–Fock approximation to calculate the rich phase diagram of CTTBG at all integer and half-integer fillings in both stacking orders and under the vertical displacement field. Under a small displacement field, the groundstates are flavor polarized states for AB-AB-BC stacking order and intervalley coherent states for AB-AB-AB stacking order at all integer and half-integer fillings. A larger displacement field will turn them into layer-polarized states. At half-integer fillings, the groundstates also exhibit charge density wave (CDW) order. For AB-AB-AB stacking, the groundstates at half-integer fillings are always 2 × 1 stripe state among a range of displacement fields. For AB-AB-BC stacking, the groundstates at half-integer fillings are also 2 × 1 stripe states under a small displacement field and a larger displacement will possibly favor further translation-symmetry-breaking, depending on filling and the direction of the displacement field. We demonstrate that the CDW states observed in the experiment can originate from the strong Coulomb interaction of the flat band electrons.
受最近在啁啾扭曲三重双层石墨烯(CTTBG)的整数和半整数填充处观察到的位移场调谐相关绝缘体的实验结果[Phys.Rev.Lett.132.246501]的激励,我们研究了 CTTBG 的单粒子和相互作用物理。我们发现存在两种不等价的堆叠阶,即 AB-AB-BC 和 AB-AB-AB,并且两者都表现出具有非难拓扑的平坦带。然后,我们使用哈特里-福克近似法计算了 CTTBG 在两种堆叠阶的所有整数和半整数填充以及垂直位移场下的丰富相图。在小位移场下,AB-AB-BC 堆积阶的基态是风味极化态,而在所有整数和半整数填充下,AB-AB-AB 堆积阶的基态是间隔相干态。较大的位移场将使它们变成层极化态。在半整数填充时,基态也表现出电荷密度波(CDW)阶。对于 AB-AB-AB 堆叠,半整数填充时的基态在一系列位移场中总是 2 × 1 条纹态。对于 AB-AB-BC 堆叠,在小位移场下,半整数填充的基态也是 2 × 1 条纹态,而较大的位移则可能有利于进一步的平移对称性破缺,这取决于填充和位移场的方向。我们证明,实验中观察到的 CDW 状态可能源于平带电子的强库仑相互作用。
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引用次数: 0
Quantum machine learning for corrosion resistance in stainless steel 针对不锈钢耐腐蚀性的量子机器学习
Pub Date : 2024-09-01 DOI: 10.1016/j.mtquan.2024.100013
Muhamad Akrom , Supriadi Rustad , Totok Sutojo , De Rosal Ignatius Moses Setiadi , Hermawan Kresno Dipojono , Ryo Maezono , Moses Solomon

This study evaluates the efficacy of quantum machine learning (QML) models in predicting stainless steel corrosion behaviour. Using two datasets, the quantum support vector classifier (QSVC) outperformed classical models, achieving accuracies of 95.46 % and 94.80 % for Dataset A and Dataset B, respectively. The QSVC excelled in identifying complex corrosion classes and demonstrated robust performance across diverse environments. This QML approach accurately predicts corrosion without experimental testing, saving significant time and cost. Future research will aim to include more environmental variables and steel types, broadening the model's applicability.

本研究评估了量子机器学习(QML)模型在预测不锈钢腐蚀行为方面的功效。利用两个数据集,量子支持向量分类器(QSVC)的表现优于经典模型,数据集 A 和数据集 B 的准确率分别达到 95.46 % 和 94.80 %。QSVC 在识别复杂的腐蚀类别方面表现出色,并在不同环境下表现出稳健的性能。这种 QML 方法无需实验测试即可准确预测腐蚀,从而节省了大量时间和成本。未来的研究将致力于纳入更多的环境变量和钢材类型,从而扩大模型的适用性。
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引用次数: 0
Layer-polarized anomalous Hall effect in the MnBi2Te4/In2Se3 (In2Te3) heterostructures MnBi2Te4/In2Se3 (In2Te3) 异质结构中的层极化反常霍尔效应
Pub Date : 2024-09-01 DOI: 10.1016/j.mtquan.2024.100012
Hong Xu, Xuqi Li, Haidan Sang, Yu Zhang, Wenying Mu, Shifei Qi
<div><p>The layer-polarized anomalous Hall effect has emerged as a novel phenomenon in the field of condensed matter physics, holding significant promise for future applications in designing low-dissipation devices. Currently, the layer-polarized anomalous Hall effect has been theoretically predicted or experimentally demonstrated through the application of external electric fields or the utilization of sliding ferroelectricity in diverse systems. Here, through first-principles calculations, we propose a pathway to realize the layer-polarized anomalous Hall effect by constructing A-type antiferromagnetic topological insulator MnBi<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>4</mn></mrow></msub></math></span> based heterostructures with ferroelectric materials In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Se<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span>/In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span>. Our results firstly show that the sizeable band splitting (larger than 20 meV) appears in the antiferromagnetic 4 septuple layers MnBi<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>4</mn></mrow></msub></math></span>/In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Se<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> system due to broken inversion symmetry. Further calculations approve that the layer-polarized anomalous Hall conductivity with reversal signs can be observed in the antiferromagnetic 4 septuple layers MnBi<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>4</mn></mrow></msub></math></span>/In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Se<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> (In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span>) systems by shifting the Fermi energy level. Additionally, it is also found that ferrimagnetic 4 septuple layers MnBi<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>4</mn></mrow></msub></math></span>/In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Se<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span> (In<span><math><msub><mrow></mrow><mrow><mn>2</mn></mrow></msub></math></span>Te<span><math><msub><mrow></mrow><mrow><mn>3</mn></mrow></msub></math></span>) can be realized by controlling the direction of ferroelectric polarization of ferroelectric materials. Thus, the resulting layer-polarized anomalous Hal
层极化反常霍尔效应是凝聚态物理领域出现的一种新现象,在未来设计低耗散器件的应用中大有可为。目前,层极化反常霍尔效应已通过外加电场或利用不同系统中的滑动铁电现象得到理论预测或实验证明。在此,我们通过第一性原理计算,提出了一种通过构建基于 A 型反铁磁拓扑绝缘体 MnBi2Te4 与铁电材料 In2Se3/In2Te3 的异质结构来实现层极化反常霍尔效应的途径。我们的研究结果首先表明,由于反转对称性被打破,反铁磁性 4 七层 MnBi2Te4/In2Se3 体系中出现了相当大的带分裂(大于 20 meV)。进一步的计算表明,通过移动费米能级,可以在反铁磁性 4 七层 MnBi2Te4/In2Se3 (In2Te3) 系统中观察到具有反转符号的层极化反常霍尔电导率。此外,研究还发现,通过控制铁电材料的铁电极化方向,可以实现铁磁性 4 七层 MnBi2Te4/In2Se3 (In2Te3)。因此,在我们建议的系统中,所产生的层极化反常霍尔效应可能是可切换的。这项工作为进一步实验实现层极化反常霍尔效应提供了可行的系统。
{"title":"Layer-polarized anomalous Hall effect in the MnBi2Te4/In2Se3 (In2Te3) heterostructures","authors":"Hong Xu,&nbsp;Xuqi Li,&nbsp;Haidan Sang,&nbsp;Yu Zhang,&nbsp;Wenying Mu,&nbsp;Shifei Qi","doi":"10.1016/j.mtquan.2024.100012","DOIUrl":"10.1016/j.mtquan.2024.100012","url":null,"abstract":"&lt;div&gt;&lt;p&gt;The layer-polarized anomalous Hall effect has emerged as a novel phenomenon in the field of condensed matter physics, holding significant promise for future applications in designing low-dissipation devices. Currently, the layer-polarized anomalous Hall effect has been theoretically predicted or experimentally demonstrated through the application of external electric fields or the utilization of sliding ferroelectricity in diverse systems. Here, through first-principles calculations, we propose a pathway to realize the layer-polarized anomalous Hall effect by constructing A-type antiferromagnetic topological insulator MnBi&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; based heterostructures with ferroelectric materials In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Se&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;. Our results firstly show that the sizeable band splitting (larger than 20 meV) appears in the antiferromagnetic 4 septuple layers MnBi&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Se&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; system due to broken inversion symmetry. Further calculations approve that the layer-polarized anomalous Hall conductivity with reversal signs can be observed in the antiferromagnetic 4 septuple layers MnBi&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Se&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; (In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) systems by shifting the Fermi energy level. Additionally, it is also found that ferrimagnetic 4 septuple layers MnBi&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;4&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Se&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; (In&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;Te&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mrow&gt;&lt;/mrow&gt;&lt;mrow&gt;&lt;mn&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;) can be realized by controlling the direction of ferroelectric polarization of ferroelectric materials. Thus, the resulting layer-polarized anomalous Hal","PeriodicalId":100894,"journal":{"name":"Materials Today Quantum","volume":"3 ","pages":"Article 100012"},"PeriodicalIF":0.0,"publicationDate":"2024-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S295025782400012X/pdfft?md5=56d493650688f0da73b3e5e4c7112299&pid=1-s2.0-S295025782400012X-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142094775","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Senna-based carbon quantum dots as probes for the determination of Fe3+ and dopamine 番泻叶基碳量子点作为测定 Fe3+ 和多巴胺的探针
Pub Date : 2024-09-01 DOI: 10.1016/j.mtquan.2024.100014
Ping Lu , Xiangru Hou , Lu Ga , Gerile Aodeng , Jun Ai

Carbon quantum dots (CQDs) are widely used in optical biosensors due to their good biocompatibility and easy synthesis type. Although the carbon sources for preparing CQDs are quite extensive, it is not common to prepare CQDs using herbs as carbon sources. Therefore, CQDs for fluorescence determination of Fe3+ and dopamine (DA) were prepared by microwave heating using senna leaf as carbon source. The prepared CQDs showed good dispersion and uniform sphericity under transmission electron microscopy (TEM), with an average particle size of 3.510 nm. Under ultraviolet light, CQDs fluoresce brightly blue and have a strong fluorescence (>1.200*103 a.u.), with no change in fluorescence intensity over a week. The prepared CQDs were quenched by Fe3+ and DA probably due to the static burst effect, which can be confirmed by X-ray photoelectron spectroscopy (XPS) and fourier-transform infrared spectroscopy (FT-IR) analyses. The method has a good linear relationship for Fe3+ in the range of 10–3000 μmol/L with a determination limit of 0.1671 μmol/L, and an excellent linear relationship for DA in the range of 5–3000 μmol/L with a determination limit of 0.1653 μmol/L. The method was applied to the determination of Fe3+ and DA in real samples, and the recovery rate was satisfactory.

碳量子点(CQDs)具有良好的生物相容性和易于合成的特点,因此被广泛应用于光学生物传感器。虽然制备 CQDs 的碳源相当广泛,但用中草药作为碳源制备 CQDs 并不常见。因此,本研究以番泻叶为碳源,通过微波加热制备了用于荧光测定 Fe3+ 和多巴胺(DA)的 CQDs。制备的CQDs在透射电子显微镜(TEM)下显示出良好的分散性和均匀的球形度,平均粒径为3.510 nm。在紫外光下,CQDs发出明亮的蓝色荧光,且荧光强度较强(1.200*103 a.u.),荧光强度在一周内无变化。制备的 CQDs 可能由于静态猝灭效应而被 Fe3+ 和 DA 所淬灭,这可以通过 X 射线光电子能谱(XPS)和傅立叶变换红外光谱(FT-IR)分析得到证实。该方法在10-3000 μmol/L范围内对Fe3+的线性关系良好,测定限为0.1671 μmol/L;在5-3000 μmol/L范围内对DA的线性关系良好,测定限为0.1653 μmol/L。应用该方法测定了实际样品中的Fe3+和DA,回收率令人满意。
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引用次数: 0
Synthesis of strongly confined Bi2Te3 quantum dots by pulsed laser ablation in liquids 通过脉冲激光烧蚀在液体中合成强约束 Bi2Te3 量子点
Pub Date : 2024-08-22 DOI: 10.1016/j.mtquan.2024.100011
Rajendra Subedi , Francisco Ruiz-Zepeda , Qiaohui Zhou , Xin Lu , Grégory Guisbiers

Quantum dots are semiconductor nanoparticles where electrons’ motion is confined within the three physical dimensions of the nanoparticle, such that discretization of energy levels is observed. In this article, quantum dots of Bi2Te3, with sizes around 9 ± 2 nm and energy bandgap around ∼ 2.8 eV, were successfully synthesized by pulsed laser ablation in liquids. Those dots were found to be within the strong confinement regime.

量子点是一种半导体纳米粒子,电子的运动被限制在纳米粒子的三个物理维度内,从而观察到能级的离散化。本文在液体中通过脉冲激光烧蚀成功合成了尺寸约为 9 ± 2 nm、能带隙约为∼ 2.8 eV 的 Bi2Te3 量子点。研究发现,这些点处于强约束状态。
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引用次数: 0
Stabilization mechanisms of magnetic skyrmion crystal and multiple-Q states based on momentum-resolved spin interactions 基于动量分辨自旋相互作用的磁性天融晶体和多Q态稳定机制
Pub Date : 2024-08-17 DOI: 10.1016/j.mtquan.2024.100010
Satoru Hayami , Ryota Yambe

Multiple-Q states as represented by a magnetic skyrmion crystal and hedgehog crystal have been extensively studied in recent years owing to their unconventional physical properties. The materials hosting multiple-Q states have been so far observed in a variety of lattice structures and chemical compositions, which indicates rich stabilization mechanisms inducing the multiple-Q states. We review recent developments in the research of the stabilization mechanisms of such multiple-Q states with an emphasis on the microscopic spin interactions in momentum space. We show that an effective momentum-resolved spin model is a canonical model for not only understanding the microscopic origin of various multiple-Q states but also exploring further exotic multiple-Q states with topological properties. We introduce several key ingredients to realize the magnetic skyrmion crystal with the skyrmion numbers of one and two, hedgehog crystal, meron–antimeron crystal, bubble crystal, and other multiple-Q states. We also review that the effective spin model can be used to reproduce the magnetic phase diagram in experiments efficiently.

近年来,以磁性天幕晶体和刺猬晶体为代表的多重Q态因其非传统的物理特性而被广泛研究。迄今为止,已观察到多种晶格结构和化学成分的材料中存在多重Q态,这表明诱导多重Q态的稳定机制非常丰富。我们回顾了此类多重 Q 态稳定机制研究的最新进展,重点关注动量空间中的微观自旋相互作用。我们表明,有效的动量分辨自旋模型是一个典型的模型,它不仅能理解各种多重 Q 态的微观起源,还能进一步探索具有拓扑特性的奇异多重 Q 态。我们介绍了实现磁性天戎晶体(天戎数为 1 和 2)、刺猬晶体、梅隆锑晶体、气泡晶体和其他多 Q 态的几个关键要素。我们还回顾了有效自旋模型可用于有效重现实验中的磁相图。
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引用次数: 0
Selective detection of Co2+ by L-CyS/AA CQDs and Construction of PASS 0 gate 用 L-CyS/AA CQDs 选择性检测 Co2+ 并构建 PASS 0 门
Pub Date : 2024-07-23 DOI: 10.1016/j.mtquan.2024.100009
Lijun Liu , Xiangru Hou , Gerile Aodeng , Lu Ga , Jun Ai

Since the accidental discovery of carbon quantum dots (CQDs) in 2004, they have been widely used in the field of fluorescence sensing by combining their good optical and physicochemical properties with a wide source of raw materials and a simple synthesis process. In this work, we have synthesised sulphur-doped carbon quantum dots L-CyS/AA CQDs by a one-step microwave method using L-cysteine (L-CyS) and ascorbic acid (AA) as carbon and sulphur sources. It was also analysed by fluorescence spectroscopy, X-ray photoelectron spectroscopy (XPS) and transmission electron microscopy (TEM). The prepared L-CyS/AA CQDs showed good dispersion under TEM with a spherical shape and an average particle size of 7.3 nm. L-CyS/AA CQDs were observed to be bright blue-green fluorescent with strong fluorescence (>3.5*103 a.u.) under UV light irradiation. PASS 0 logic gate operation can be achieved by controlling different fluorescent input and output. L-CyS/AA CQDs were able to achieve selective detection of Co2+ with a LOD of 63.2 μM, which provides a new method for Co2+ detection that can be used for the detection of Co2+ in real water samples.

碳量子点(CQDs)自 2004 年被意外发现以来,凭借其良好的光学和物理化学特性、广泛的原料来源和简单的合成工艺,已被广泛应用于荧光传感领域。在这项工作中,我们以 L-半胱氨酸(L-CyS)和抗坏血酸(AA)为碳源和硫源,通过一步微波法合成了掺硫的碳量子点 L-CyS/AA CQDs。此外,还利用荧光光谱、X 射线光电子能谱(XPS)和透射电子显微镜(TEM)对其进行了分析。制备的 L-CyS/AA CQDs 在 TEM 下显示出良好的分散性,呈球形,平均粒径为 7.3 nm。在紫外光照射下,观察到 L-CyS/AA CQDs 发出明亮的蓝绿色荧光,荧光强度高(3.5*103 a.u.)。通过控制不同的荧光输入和输出,可以实现 PASS 0 逻辑门操作。L-CyS/AA CQDs能够实现对Co2+的选择性检测,LOD为63.2 μM,这为Co2+的检测提供了一种新方法,可用于实际水样中Co2+的检测。
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Materials Today Quantum
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