中空多壳层结构在电磁波领域中的应用

中空多壳层结构(HoMSs)是一种以纳米颗粒为结构单元构筑而成的具有多界面、 多维度的微纳米级宏观组装体, 具有次序排列的多个壳层及相互连通的多个空腔, 被认为是电磁波领域极具应用前景的功能材料. 本文主要从电磁波捕获、 传输及能量转换3个角度详细阐述HoMSs在电磁波领域应用中的独特优势, 浅析了HoMSs壳层数目、 壳层厚度、 壳层间距、 壳层组成等结构参数对电磁波传输与利用的影响规律, 并预测了HoMSs在电磁波领域的发展趋势, 以期为实现电磁波的高效利用提供参考.     

监控系统预警视频的分布式检索设计与实现

视频监控系统在日积月累的监控过程中会产生大量的视频信息,如何在海量视频中基于内容快速检索出需要的信息成为亟待解决的问题;文章在视频检索过程中,将视频图像的SIFT特征提取匹配与MapReduce并行模式相结合,同时利用LSH映射对视频图像进行分组并存储在HBase数据库中,在配合并行分析的同时减少了计算量;最后实验证明,采用MapReduce并行模式提取图像SIFT特征值,时间会随着集群节点的增加而不断降低,并最终趋于稳定;由此可知,对基于内容的视频检索采用并行化分析可以显著提高效率,实现了Hadoop架构在视频分析方面的应用拓展。     

对一道经典折叠压轴题的探析与建议

一、问题呈现题目平面直角坐标系中有一张矩形纸片OABC,O为坐标原点,A点坐标为(10,0),C点坐标为(0,8),D是线段AB上的一点,沿直线CD折叠矩形OABC的一边BC,使点B落在OA边上的点E处(如图1),有一抛物线y=ax2+bx+c(a、b、c是常数,且a≠0)经过O、C、D三点.(1)求线段AD的长及抛物线的解析式     

TiO2/Fe2O3异质结薄膜的制备及其光电特性的研究

通过水热法成功在FTO上制得Ti O2/Fe2O3异质结薄膜,采用场发射扫描电子显微镜(FESEM)、X射线衍射仪(XRD)、紫外-可见吸收光谱(UV-Vis)分析测试手段对样品的形貌和结构进行了表征。结果表明,Ti O2/Fe2O3异质结是由直径约200~300 nm的Ti O2纳米棒镶嵌着Fe2O3纳米颗粒组成。通过光电流测试,证明Ti O2/Fe2O3异质结的可见光光电转换效率相比Ti O2明显提高,并对Ti O2/Fe2O3异质结的光电转换机理进行了分析。     

空心结构NaYF4∶Yb,Er上转换材料的制备

以稀土三氟乙酸盐、氟化钠和三氟乙酸钠为原料通过溶剂热法成功制备出了空心结构的Na YF4∶Yb,Er上转换材料,探索了反应温度、钠离子浓度对产物形貌、晶相及发光性能的影响。利用扫描电镜,透射电镜,X射线衍射和发光光谱对产物的形貌、物相结构及荧光性能进行表征。结果表明,当Na F和Y3+的摩尔比为2.5,220℃溶剂热反应12 h时,可得到空心结构的上转换材料,该结构兼具上转换荧光、载药双重功能。     

新疆理化所提出一种基于模拟的使非线性光学晶体材料相匹配区间蓝移的方案

非线性光学晶体是通过频率转换拓宽固态激光器输出波段的关键材料。随着激光微加工,激光通讯和现代科学仪器的持续发展,对紫外/深紫外非线性光学晶体的需求日益增加。但是,很多拥有宽的紫外透过范围和大的倍频效应的晶体因其双折射无法满足深紫外相匹配而无法输出深紫外激光。     

具有红光发射的稀土上转换发光纳米晶及其介孔直接功能化

红光发射稀土上转换发光纳米晶(UCNPs)在光动力治疗(PDT)等方面具有特定的优势。将油溶性的UCNPs通过表面改性转变为水溶性,对其在生物医疗、疾病诊断等方面的应用具有重要意义。利用一种简单易行的方法将具有红光发射的UCNPs进行介孔直接功能化表面修饰,制备了一种具有良好水溶性的纳米材料NaYF4:Yb/Er/Mn@mSiO2。实验结果表明该材料核-壳结构明显,形貌均一,在980 nm的激发下保持了上转换发光特性。该材料在光动力治疗等方面具有良好的潜在应用价值。     

光催化合成金属Ag纳米颗粒的生长机制——晶核密度控制的生长模式转换

利用AgNO3水溶液,通过严格控制TiO2薄膜的化学活性,系统研究了在TiO2表面光催化合成金属Ag纳米颗粒的生长行为。研究发现,光催化合成金属Ag纳米颗粒存在着两个完全不同的生长机制,分别对应着金属Ag纳米颗粒的各向同性和各向异性生长。当溶液浓度较低时,Ostwald熟化(OR)机制主导着金属Ag纳米颗粒的长大过程;当溶液浓度较高时,取向附生(OA)机制决定着金属Ag纳米颗粒长大成纳米片。原位消光光谱分析表明,OR机制和OA机制生长的前期具有相近消光特征,决定金属Ag纳米颗粒生长模式的关键是AgNO3溶液的浓度,更准确地说是金属Ag初级晶核的局域密度。在此基础上提出了有关光催化合成金属Ag纳米颗粒的生长模型。     

Synthesis,Crystal Structure and Photoluminescence of a Three-coordinate Ag(Ⅰ) Complex

A three-coordinate Ag(I) complex, [Ag(Mepzpy)(PAr3)]BF4·H2O(1, Mepzpy = 3-methyl-1-(2-pyridyl)pyrazole, PAr3 = tri(o-tolyl)phosphine), was synthesized from the reaction of Ag(CH3CN)4BF4, PAr3 and Mepzpy in CH3 CN at room temperature. The compound was characterized by UV-vis, NMR and X-ray single-crystal structure analysis. It crystallizes in triclinic space group P1 with a = 10.2251(5), b = 10.6014(5), c = 15.7012(5) , α = 92.963(3), β = 92.641(3), γ = 114.647(4)o, V = 1540.6(1) 3, Z = 2, Mr = 676.24, Dc = 1.458 g/cm3, F(000) = 688, μ = 6.187 mm-1, GOOF = 1.038, the final R = 0.0530 and w R = 0.1493 for 6371 observed reflections with I 2σ(I). Compound 1 is ionic. It is composed of a BF4- anion and a [Ag(Mepzpy)(PAr3)]+ cation. The Ag(I) ion adopts a distorted trigonal pyramidal coordination geometry defined by two nitrogen atoms and a phosphorous atom. The complex emits blue luminescence with maximum peaks at 470 nm in solid state at room temperature.     

基于上转换纳米粒子的低损伤神经界面技术

Optogenetics is a neuromodulation technology that combines light control technology with genetic technology, thus allowing the selective activation and inhibition of the electrical activity in specific types of neurons with millisecond time resolution. Over the past several years, optogenetics has become a powerful tool for understanding the organization and functions of neural circuits, and it holds great promise to treat neurological disorders. To date, the excitation wavelengths of commonly employed opsins in optogenetics are located in the visible spectrum. This poses a serious limitation for neural activity regulation because the intense absorption and scattering of visible light by tissues lead to the loss of excitation light energy and also cause tissue heating. To regulate the activity of neurons in deep brain regions, it is necessary to implant optical fibers or optoelectronic devices into target brain areas, which however can induce severe tissue damage. Non- or minimally-invasive remote control technologies that can manipulate neural activity have been highly desirable in neuroscience research. Upconversion nanoparticles (UCNPs) can emit light with a short wavelength and high frequency upon excitation by light with a long wavelength and low frequency. Therefore, UCNPs can convert low-frequency near-infrared (NIR) light into high-frequency visible light for the activation of light-sensitive proteins, thus indirectly realizing the NIR optogenetic system. Because NIR light has a large tissue penetration depth, UCNP-mediated optogenetics has attracted significant interest for deep-tissue neuromodulation. However, in UCNP-mediated in vivo optogenetic experiments, as the up-conversion efficiency of UCNPs is low, it is generally necessary to apply high-power NIR light to obtain up-converted fluorescence with energy high enough to activate a photosensitive protein. High-power NIR light can cause thermal damage to tissues, which seriously restricts the applications of UCNPs in optogenetic technology. Therefore, the exploration of strategies to increase the up-conversion efficiency, fluorescence intensity, and biocompatibility of UCNPs is of great significance to their wide applications in optogenetic systems. This review summarizes recent developments and challenges in UCNP-mediated optogenetics for deep-brain neuromodulation. We firstly discuss the correspondence between the parameters of UCNPs and employed opsins in optogenetic experiments, which mainly include excitation wavelengths, emission wavelengths, and luminescent lifetimes. Thereafter, we introduce the methods to enhance the conversion efficiency of UCNPs, including optimizing the structure of UCNPs and modifying the organic dyes in UCNPs. In addition, we also discuss the future opportunities in combining UCNP-mediated optogenetics with flexible microelectrode technology for the long-term detection and regulation of neural activity in the case of minimal injury.