CTA在急性复杂性大咯血患者行介入栓塞术前的应用价值分析

本文探讨了CT血管造影(CT angiography,CTA)在急性复杂性大咯血患者行介入栓塞术前的应用价值。回顾性选择49例急性复杂性大咯血患者CTA影像资料,通过与术中数字减影血管造影(digital subtraction angiography,DSA)结果进行对比,发现CTA对罪犯血管诊断准确率为89.33%,对多动脉交通吻合诊断准确率为86.96%。Kappa检验CTA与DSA检查结果一致性较高,受试者特征曲线(ROC)分析CTA诊断急性复杂性大咯血罪犯血管的曲线下面积(AUC)为0.947(95%CI:0.903~0.990,P=0.000),灵敏度89.33%,特异度100.00%。通过随访发现CTA指导下行介入栓塞术治疗有效率91.84%,术后1年无大咯血复发病例。     

超微血管成像和超声造影对乳腺癌病灶内微血流及超微血管的评价及其联合诊断价值

本文探讨了超微血管成像(SMI)和超声造影(CEUS)对乳腺癌病灶内微血流及超微血管的评价,及其联合检查对乳腺癌的诊断价值。选取2017年6月~2019年3月我院收治的经手术病理证实的乳腺癌患者106例(106个肿块)作为研究对象,所有患者术前均完成彩色多普勒血流显像(CDFI)、CEUS及SMI检查。比较SMI、CEUS对乳腺癌的诊断准确率及对病灶内血流信号、穿支血管的显示情况。结果显示,106例乳腺癌(106个肿块)中,SMI和CEUS对乳腺癌的诊断准确率分别为79.25%、83.96%,两者比较差异无统计学意义(P>0.05);SMI联合CEUS检查对乳腺癌的诊断准确率为96.23%,明显高于单一SMI或CEUS的诊断准确率(P<0.05)。在血流信号显示上,SMI检出不丰富血流信号、丰富血流信号分别为64个、42个;CEUS表现为低增强64个、等增强及高增强为42个;SMI和CEUS评价乳腺癌病灶内微血管及血流供应情况具有较好的一致性(P<0.05)。在穿支血管显示上,SMI检出44个、CDFI检出34个,SMI能够清晰检出CDFI不能检出的穿支血管10个。表明SMI和CEUS诊断乳腺癌病灶内微血管及血流供应情况具有较好的一致性,对乳腺癌均有较高的诊断价值,二者联合检查有助于提高乳腺癌的诊断准确率。     

SBFEM与非局部宏微观损伤模型相结合的准脆性材料开裂模拟

混凝土是一种被广泛应用于土木和水利工程中的准脆性材料, 在各种内外部因素的作用下, 开裂是混凝土结构最为普遍的破坏形式, 准确模拟结构的开裂过程, 对于结构的安全评估至关重要. 将比例边界有限元与非局部宏微观损伤模型相结合提出一种准脆性材料开裂模拟新方法. 以比例边界有限元子域的比例中心作为物质点, 通过两比例中心(物质点对)之间的物质键的正伸长率来定义微细观损伤, 将某点影响域内物质键的微细观损伤加权平均得到该点的宏观拓扑损伤. 再引入能量退化函数, 将宏观拓扑损伤嵌入到比例边界有限元的基本框架中. 充分利用比例边界有限元网格允许存在悬挂节点的优势, 采用四叉树网格离散技术进行快速、高质量的多级网格划分与过渡. 通过一个I型开裂与一个混合型开裂的两个典型算例, 验证了该方法可捕获结构裂纹扩展路径与荷载变形曲线. 与现有的方法相比, 本文的损伤模型可得到更准确的局部开裂损伤带, 结果更为合理, 且具有更高的计算精度和计算效率. 当损伤过程区网格尺寸小于影响域半径的1/5时, 计算结果不存在网格敏感性问题.      

LOCAL BENDING OF THIN FILM ON VISCOUS LAYER

Effects of deposition layer position film are systematically investigated. Because the and number/density on local bending of a thin deposition layer interacts with the thin film at the interface and there is an offset between the thin film neutral surface and the interface, the deposition layer generates not only axial stress but also bending moment. The bending moment induces an instant out-of-plane deflection of the thin film, which may or may not cause the socalled local bending. The deposition layer is modeled as a local stressor, whose location and density are demonstrated to be vital to the occurrence of local bending. The thin film rests on a viscous layer, which is governed by the Navier-Stokes equation and behaves like an elastic foundation to exert transverse forces on the thin film. The unknown feature of the axial constraint force makes the governing equation highly nonlinear even for the small deflection chse. The constraint force and film transverse deflection are solved iteratively through the governing equation and the displacement constraint equation of immovable edges. This research shows that in some special cases, the deposition density increase does not necessarily reduce the local bending. By comparing the thin film deflections of different deposition numbers and positions, we also present the guideline of strengthening or suppressing the local bending.     

多元Copula密度估计的小波局部阈值方法

为了量化资产之间相依结构的局部特征,本文将小波阈值规则引入Copula参数估计,提出多元Copula密度的小波局部阈值估计量,发现Copula密度的光滑度指数、维数和采样容量是影响估值精度的重要因素,这一点也得到了以正态Copula为仿真算例的支持。本方法增强了参数Copula建模的局部自适应能力,进而有助于改进资产的市场风险估值与最优化配置。     

LOCALLY STABILIZED FINITE ELEMENT METHOD FOR STOKES PROBLEM WITH NONLINEAR SLIP BOUNDARY CONDITIONS

Based on the low-order conforming finite element subspace （Vh, Mh） such as the P1-P0 triangle element or the Q1-P0 quadrilateral element, the locally stabilized finite element method for the Stokes problem with nonlinear slip boundary conditions is investigated in this paper. For this class of nonlinear slip boundary conditions including the subdifferential property, the weak variational formulation associated with the Stokes problem is an variational inequality. Since （Vh, Mh） does not satisfy the discrete inf-sup conditions, a macroelement condition is introduced for constructing the locally stabilized formulation such that the stability of （Vh, Mh） is established. Under these conditions, we obtain the H1 and L2 error estimates for the numerical solutions.     

具有非局部时滞的扩散Nicholson苍蝇方程的波前解

研究了具有非局部时滞的扩散Nicholson苍蝇方程,其中时滞由一个定义在所有过去时间和整个一维空间区域上的积分卷积表示.当时滞核是强生成核时,根据线性链式技巧和几何奇异扰动理论,获得了小时滞时波前解的存在性.     

块体金属玻璃的剪切带行为

0 引言 玻璃态物质以纷繁多样的形式广泛存在于自然与科技技术领域[1-3].除了人们熟知的门窗上的硅酸盐无机玻璃、各种塑料制品的高聚物玻璃外,玻璃态还与光纤通讯、生物制品和生化药剂的保鲜存储、极端干燥条件下昆虫活性的保持等这些鲜为人知的方面密切相关.     

On the order of summability of the Fourier inversion formula

In this article we show that the order of the point value, in the sense of Łojasiewicz, of a tempered distribution and the order of summability of the pointwise Fourier inversion formula are closely related. Assuming that the order of the point values and certain order of growth at infinity are given for a tempered distribution, we estimate the order of summability of the Fourier inversion formula. For Fourier series, and in other cases, it is shown that if the distribution has a distributional point value of order k, then its Fourier series is e.v. Cesàro summable to the distributional point value of order k+1. Conversely, we also show that if the pointwise Fourier inversion formula is e.v. Cesàro summable of order k, then the distribution is the (k+1)-th derivative of a locally integrable function, and the distribution has a distributional point value of order k+2. We also establish connections between orders of summability and local behavior for other Fourier inversion problems.     

Characterizing localization properties of two spinless electrons in a one-dimensional Harper model with concurrence

By mapping the Fock space of many local fermionic modes isomorphically onto a many-qubit space and using the measure of concurrence, this paper studies numerically the mode entanglement of two spinless electrons with on-site interaction U moving in the one-dimensional Harper model. Generally speaking, for electrons in extended regimes （potential parameter λ 〈 2）, the spectrum-averaged concurrence N（C） first decreases slowly as A increases until its local minimum, then increases with λ until its peak at λ = 2, while for electrons in localized regimes （λ 〉 2）, N（C） decreases drastically as λ increases. The functions of N（C） versus λ are different for electrons in extended and localized regimes. The maximum of N（C） occurs at the point λ= 2, which is the critical value in the one-dimensional singleparticle Harper model. From these studies it can distinguish extended, localized and critical regimes for the two-particle system. It is also found for the same λ that the interaction U always induce the decreases of concurrence, i.e., the concurrence can reflect the localization effect due to the interaction. All these provide us a new quantity to understand the localization properties of eigenstates of two interacting particles.