基于单幅散斑的X射线强度关联缺陷检测方法

采用预置散斑的X射线强度关联成像系统需要采集大量的散斑场,成像时间较长,而单幅散斑场信噪比低,难以单独用于图像重构。然而单幅散斑场中的空间分布信息包含一定的样品结构信息,可以用于样品缺陷快速检测。基于此,提出一种基于单幅预置散斑的缺陷检测方法,该方法将待检测样品探测散斑场与标准样品模拟散斑场的相关性作为样品缺陷的评价标准。同时基于该方法模拟X射线强度涨落二阶自关联检测光路,分析不同信噪比下探测散斑场分布的图像对比度对相关系数的影响。并对比多种细节增强方法,提高检测可靠性。最终结果表明,基于单幅散斑场的方法可以有效地进行样品的快速缺陷检测。     

CBMT测井数值模拟及水泥环第二界面成像

从油田开发实际情况来看,在第一界面胶结良好的井段进行射孔,会因第二界面胶结差引起部分地层间流体窜槽,因此,研究第二界面胶结质量的评价方法是一项急需解决的工作。本文在中海油服自主研发的扇区水泥胶结成像测井仪器 CBMT 基础上,采用反褶积等算法,对数值模拟的CBMT 仪器贴井壁测量的全波波形进行水泥环第二界面成像处理,并分析第一界面、第二界面不同胶结情况下的成像效果。通过成像分析得出,在水泥环第一界面胶结良好时,可以对水泥环第二界面胶结状况较好地成像;在水泥环第一界面胶结差时,较难评价水泥环第二界面的胶结状况。     

壳聚糖的改性及其纳米粒子的制备

通过壳聚糖上的氨基与硬脂酸和硫辛酸的羧基脱水缩合反应,将硬脂酸和硫辛酸接枝在壳聚糖上,引入的疏水性基团使修饰的壳聚糖具有两亲性。对修饰壳聚糖残留的自由氨基进行甲基化,使氨基的pKa值由6.6增加到6.8~7.1。修饰的壳聚糖在水介质中经超声分散即可形成纳米粒子,纳米粒子的Zeta电位为正值,说明修饰壳聚糖中残留的氨基和甲基化的氨基处于纳米粒子的表面。纳米粒子经二硫苏糖醇还原,然后经空气中的氧气氧化,在纳米粒子中形成二硫键交联结构。     

基于适体竞争机理的溶菌酶电化学传感器

制备了基于溶菌酶适体竞争机理的信号减弱型电化学传感器,在玻碳电极上修饰羧基化的多壁碳纳米管,将带有氨基的互补适体DNA连接到多壁碳纳米管上。由于道诺霉素崁入电极上的互补DNA,而产生电化学信号,当有目标物时,适体与结合力更高的溶菌酶结合,原本的互补链解链,导致插入双链的道诺霉素脱落,电化学信号减弱。以微分脉冲伏安法测定溶菌酶,响应的范围为1～500 nmol/L,相关系数0.999,检测下限为0.5 nmol/L(S/N=3)。     

模型多肽Trp-Cage折叠形成机制的研究进展

蛋白质折叠是目前结构生物学领域的核心问题之一, 理解蛋白质结构折叠机制及其与生物功能之间的相互关系一直是生命科学家非常重要的研究内容, 并且该研究受到越来越多不同学科领域研究工作者的高度重视. 蛋白质大多数在数十毫秒、微秒或几秒内完成自我折叠过程, 但其折叠过程中所发生的分子结构精细转变却在纳秒甚至更短时间尺度内完成. 由于其折叠时间分辨率的限制, 目前无论是从常规实验还是理论计算角度对其研究都存在一定的难度. 本文首先概述了蛋白质折叠研究在实验和理论模拟方面存在的一些问题,然后以结构典型且可快速折叠的人工设计多肽Trp-cage为例,主要对其折叠过渡温度、折叠形成模型及其肽链上关键氨基酸残基在折叠过程中的作用三个方面进行了详细讨论, 综述了模型多肽Trp-cage的折叠动力学行为分别在实验和理论模拟方面的研究进展. 最后就如何有效化解蛋白质残基间相互作用网络进而降低其折叠机制的复杂性提出了一些新的建议, 不仅有助于阐明该迷你蛋白Trp-cage快速折叠、稳定形成的驱动力成因, 而且也能为蛋白质折叠机制研究和多肽设计提供有益参考.     

Preparation of single-hole hollow polymer nanospheres by raspberry-like template method

Single-hole hollow polymer nanospheres were fabricated by raspberry-like template method using "graft-from" strategy through atom transfer radical polymerization (ATRP). Nanometer-sized silica spheres were covalently attached onto the surfaces of micrometer-sized silica spheres. Crosslinked polymer shells on the nano-sized spheres outside the attached area were formed by "graft-from" strategy through ATRP. After removal of the silica cores, single-hole hollow crosslinked polymer nanospheres were obtained. In this strategy, most of ATRP monomers may be used and thus many functional groups can be easily incorporated into the single-hole hollow crosslinked polymer nanospheres.     

Connes distance of 2D harmonic oscillators in quantum phase space

We study the Connes distance of quantum states of two-dimensional (2D) harmonic oscillators in phase space. Using the Hilbert-Schmidt operatorial formulation, we construct a boson Fock space and a quantum Hilbert space, and obtain the Dirac operator and a spectral triple corresponding to a four-dimensional (4D) quantum phase space. Based on the ball condition, we obtain some constraint relations about the optimal elements. We construct the corresponding optimal elements and then derive the Connes distance between two arbitrary Fock states of 2D quantum harmonic oscillators. We prove that these two-dimensional distances satisfy the Pythagoras theorem. These results are significant for the study of geometric structures of noncommutative spaces, and it can also help us to study the physical properties of quantum systems in some kinds of noncommutative spaces.     

Klein Paradox of Two-Dimensional Dirac Electrons in Circular Well Potential

We study two-dimensional massive Dirac equation in circular well potential. The energies of bound states are obtained. We demonstrate the Klein paradox of this relativistic wave equation:For large enough potential depth, the bound states disappear from the spectra. Applications to graphene systems are discussed.     

Microcanonical Phase Diagram of the BEG and Ising Models

The density of states of long-range Blume-Emery-Griffiths(BEG) and short-range Ising models are obtained by using Wang-Landau sampling with adaptive windows in energy and magnetization space.With accurate density of states,we are able to calculate the microcanonical specific heat of fixed magnetization introduced by Kastner et al.in the regions of positive and negative temperature.The microcanonical phase diagram of the Ising model shows a continuous phase transition at a negative temperature in energy and magnetization plane.However the phase diagram of the long-range model constructed by peaks of the microcanonical specific heat looks obviously different from the Ising chart.     

关于热力学和统计物理学中的负温度

近年来在与多位中学物理教师接触的过程中,只要一提到"负温度"这个名词,多数都会回答"闻所未闻",或感到迷惑和神秘莫测.为弥补这种缺陷,值此《物理通报》出版30周年之际,特献上此文供中学物理教师一阅.1问题的提出其实,早在20世纪40年代,在前苏联理论物理大师朗道及其弟子栗弗席兹合著《理论物理学》丛