灰毛大青黄酮苷的分析方法和提取工艺

采用紫外分光光度法、硝酸铝-亚硝酸钠法和高效液相色谱法分别测定了灰毛大青黄酮苷含量,通过正交试验研究了灰毛大青黄酮苷提取工艺.试验结果表明3种分析方法结果相差较大,通过测定机理分析,确立了硝酸铝-亚硝酸钠法为灰毛大青黄酮苷含量测定的适宜方法,3种方法都具有较好的线性关系,精密度、稳定性、重现性和回收率均符合要求;正交试验的适宜工艺条件为料液比1∶6 （g/V）、提取温度70℃、提取时间60min和提取次数3次,在此条件下黄酮苷得率为9.9330mg/g.     

旋转体系中湍流的LBM模拟

采用基于多松弛时间因子的格子Boltzmann方法对旋转体系中的湍流进行数值研究,考察Rossby数和Ekman数对湍流的影响,包括湍流能量及其耗散率、速度、涡结构及湍流的耗散尺度即Kolmorogov尺度和积分尺度等.研究表明,系统的旋转延缓了湍流能量的衰减速率,逐步破坏初始涡结构的均匀性,与旋转方向相反的涡逐步被抑制,并最终形成若干与旋转同向的涡柱.结果还表明,系统旋转越快,湍流的耗散尺度越小而积分尺度越大.     

二维铁电材料ABP2X6内在极高的负泊松比

Recently, ferroelectric materials have attracted considerable research attention. In particular, two dimensional (2D) ferroelectric materials have been considered as most crucial for next-generation circuit designs because of their application as novel electric memory devices. However, a 2D ferroelectric material is very rare. The ferroelectric materials with the form ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se) are of interest because of their ferroelectric property maintained in their ultrathin structures. Within the ABP₂X₆ monolayer, the P―P bonds form the pillars that hold the top and bottom X planes, while the off-center A―B atoms between the X layers induce a spontaneous ferroelectric polarization. If the two off-center A―B sites are equally aligned, this would lead to the appearance of the paraelectric state. Such intriguing structures must impart novel mechanical properties to the materials. Until now, there has been no report on the mechanical properties of monolayer ABP₂X₆. Based on first-principles calculations, we studied the structural, electronic, mechanical as well as the electromechanical coupling properties of monolayer ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se). We found that they are all semiconductors with wide bandgaps of 2.73, 2.17, 3.00, and 2.31 eV for CuInP₂Se₆, CuBiP₂Se₆, AgBiP₂S₆, and AgBiP₂Se₆, respectively, which are calculated based on the Heyd-Scuseria-Ernzerhof (HSE) exchange correlation functional model. The conduction band minimum is mainly from p orbitals of X and B atoms, whereas the valence band maximum is due to the hybridization of the p orbital of X atoms and the d orbital of A atoms. Moreover, there are three short and three long A/B―X bonds due to the A―B off-center displacement. Together with the d-p orbital hybridization, the main reason for the distorted ferroelectric structure in ABP₂X₆ monolayers is the Jahn-Teller effect. ABP₂X₆ monolayers are predicted to be a new class of auxetic materials with an out-of-plane negative Poisson's ratio, i.e., the values of the negative Poisson's ratio are in the order AgBiP₂S₆ (−0.805) < AgBiP₂Se₆ (−0.778) < CuBiP₂Se₆ (−0.670) < CuInP₂S₆ (−0.060). This is mainly due to the tensile strain applied in the x/y direction enlarging the angle between P―P bonds and top layer X atoms, thereby enhancing the bucking height of monolayer ABP₂X₆. Moreover, external strain has a significant impact on the A―B off-center displacement, rendering an out-of-plane piezoelectric polarization. The values of e₁₃ for CuInP₂S₆, CuBiP₂Se₆, AgBiP₂S₆, AgBiP₂Se₆ monolayers are calculated to be −3.95 × 10⁻¹², −5.68 × 10⁻¹², −3.94 × 10⁻¹², −2.71 × 10⁻¹² C∙m⁻¹, respectively, which are comparable to the only experimentally confirmed 2D out-of-plane piezoelectric Janus system (piezoelectric coefficient = −3.8 × 10⁻¹² C∙m⁻¹). This unusual auxetic behavior, ferroelectric polarization, and the electromechanical coupling in monolayer ABP₂X₆ could potentially lead to enormous technologically important applications in nanoelectronics, nanomechanics, and piezoelectrics.     

新型异噁唑拼接3,3'-吡咯螺环双氧化吲哚类化合物的无催化剂合成

以3-异硫氰氧化吲哚与硝基异噁唑缩合的3-烯氧化吲哚,在二氯甲烷中无催化剂条件下于室温发生Michael加成环化反应,获得了8个未见文献报道的异噁唑拼接3,3′ 吡咯螺环双氧化吲哚类化合物（3a~3h）,产率91%~95%,dr值5/3~3/1,其结构经¹H NMR, ¹³C NMR和HR-MS（ESI-TOF）表征。     

双模场与V型三能级原子玻色-爱因斯坦凝聚体相互作用系统的光场压缩效应

研究了V型三能级原子玻色-爱因斯坦凝聚体与双模压缩相干态光场相互作用系统中的光场压缩的特性.数值计算结果表明:光场的正交分量呈现周期性压缩,其周期与原子间相互作用密切相关,而最大压缩量与持续时间与初始光场的压缩因子有关.     

低磁控溅射率MCP防离子反馈膜工艺研究

为消除反馈正离子对三代微光夜视器件光阴极的有害轰击,提高微光像增强器的工作寿命,开展了低磁控溅射率法沉积微通道板（MCP）Al₂O₃防离子反馈膜的工艺研究。通过优化制备工艺,获得了制备MCP防离子反馈膜的最佳沉积条件：溅射电压1000V,溅射气压(4～5)×10^-2 Pa,沉积速率0.5nm/min等。研究结果表明：在此工艺条件下,能够制备出均匀、致密且通孔满足质量要求的MCP防离子反馈膜。如果偏离这一最佳工艺条件,制备出的MCP防离子反馈膜膜层疏松、不连续,且通孔不能满足要求。     

基于OpenCV的运动目标光流算法仿真

提出一种基于OpenCV图像库的运动目标处理算法仿真方法,介绍了OpenCV库的特点和VC6环境下的配置,通过调用库中的视频读写函数、图像特征计算和光流计算函数,得到运动目标的光流场,为运动目标状态分析和跟踪提供了基础,仅在图像库的基础上编写了少量代码就使算法得以实现,提高了编程效率。     

基于摄动法的压敏储层非线性渗流问题研究

研究地层压力变化对渗流特征的影响,对低渗透储层、碳酸盐岩储层,或其他致密性储层的油气开采和储层改造都具有重要意义.在考虑渗流压力梯度平方项存在的前提下,运用摄动法求解的相关理论,将渗透率随压力的变化融入到渗流问题的求解过程中,有效地求解了该类压敏型储层的非线性渗流问题.结果表明,在实际应用中,尤其是在储层压敏性较弱的情况下,可考虑直接用0阶摄动解即可满足较好的计算精度;储层的压敏性越强,越适宜通过用摄动解的修正,来达到精确求解的目的.     

ANNIHILATION OF VERTICAL-BLOCH-LINE CHAINS IN THE WALLS OF ORDINARY HARD BUBBLES SUBJECTED TO JOINT STATIC BIAS FIELD AND IN-PLANE FIELD

For the ordinary hard bubbles(OHBs) of garnet bubble films, the annihilation of the vertical-Bloch line (VBL) chains in their walls subjected to joint static bias field H_b and in plane field H_ip was experimentally studied. The curves of two critical in-plane fields, H⁽¹⁾_ip and H′_ip, vs H_b were measured. By means of the so-called "head-cut" and "tail-cut" experiments designed in this work, it was verified that for the OHBs subjected to H_ip, their VBL chains with different lengths lose VBLs and become shorter simultaneously. It was also verified that the critical in-plane fields H⁽¹⁾_ipand H′_ip correspond to the break down of the shortest and longest VBL chains of OHBs, respectively.     

STABILITY OF SECOND KIND OF DUMBBELL DOMAINS SUBJECTED TO AN IN-PLANE FIELD AT DIFFERENT BIAS FIELDS

The softening process of the second kind of dumbbell domalns(liDs) in garnet bubble films subjected to an in-plane field H_ip at different static bias field H_b was studied experimentally. It was found that when H_b is larger, the remaining percentage of IID, R_IID, drops sharply at a certain H_ip, and with the increase of H_b the drop occurs at lower H_ip and becomes more intensive. We have confirmed that this is related to the "spontaneous-shrink" 0f IIDs, which plays an important role for the breakdown oF vertical Bloeh line chains of lids subjected to joint fields H_ip and H_b .