拉脱法测液体表面张力系数的改进

对拉脱法测定液体表面张力系数的实验作了改进．减小Ⅱ形框横丝长度L,减短Ⅱ形框侧丝长度b,对由此引出的自升现象、α的计算公式等问题进行了相应的分析和处理,使实验用液量由原来的100mL减为5mL,并且提高了测量准确度。     

13N的一个可能的类晕的质子2p态

假设¹³N是单粒子的2p态的结构,用Glauber多重散射理论计算了1GeV的质子在¹³N上弹性散射的微分截面,研究了¹³N的类晕结构.与¹³C的情况不同,虽然目前还没有关于p-¹³N弹性散射微分截面的实验材料与我们的理论结果相比较,但是这个理论结果可以作为对未来的实验测量工作的一个指导,特别是对兰州近代物理研究所的晕核实验研究工作有参考和指导价值.参照先前我们对¹³C晕核结构的理论预言和进而的实验证实,本文的计算结果清楚地表明:¹³N可能存在着一个类晕的质子皮结构.因此,实验上测量p-¹³N弹性散射的微分截面就是当前需要马上进行的一个实验研究工作.     

二氧化碳两相回路启动时的压力脉冲现象及其抑制

机械泵驱动的二氧化碳两相回路热控系统在热载荷启动时,由于蒸发段的液-汽相变需要形核而容易造成过热.本文介绍了这部分的启动实验,结果发现,采用长程毛细管结构的蒸发器对分布式热源进行集热时,在冷工况、高热载荷、低热流密度的情况下会因液一汽相变导致压力脉冲.实验还给出了简单有效的方法抑制这种脉冲的影响.     

层状钙钛矿La1.3Sr1.7Mn2-xCuxO7的磁性及电特性

通过固相反应烧结法成功制备了层状钙钛矿La1.3Sr1.7Mn2-xCuxO7多晶,主要研究了其磁电特性.结果表明,样品为Sr3Ti2O7型钙钛矿结构.随着温度的降低,其磁性经历了一个很复杂的转变过程.当x=0时,在T*=231 K出现二维短程铁磁有序,在Tc=114 K出现三维长程铁磁有序,在TN=56 K出现倾斜的反铁磁转变.当x=0.05时,Cu替代使得T*,Tc和TN减小.其电特性表明,La1.3Sr1.7Mn2-xCuxO7多晶呈现出双峰现象,这是由于钙钛矿结构锰氧化物共生现象造成的.虽然5%Cu替代,降低了金属一绝缘体转变温度,但是却增强了磁电阻效应.     

对中学物理"难学难教"现象分析

中学物理“难学难教”似乎己成为多数物理教师和学生的共识，那么物理“难学难教”的涵义是什么？中学物理包括初中物理和高中物理，是不是初中物理和高中物理都存在“难学难教”的现象？笔者做过一次问卷调查，调查对象为初中的初二、初三两个年级学生和高中的高一、高二、高三三个年级学生．调查的内容是：在数学、物理、化学三科中，你认为哪一科最难学？哪一科比较难学？哪一科容易学？认为物理最难、比较难、容易的三项统计结果如表1所示。     

颗粒物质的两个典型效应及其研究现状的分析

概述了颗粒物质领域中粮仓现象和巴西坚果效应两个典型现象及其解释理论，分析其理论的成功和不足之处，并给出了一些看法。     

多圆孔周期性银膜阵列结构的光学特性

提出一种多圆孔周期性银膜阵列结构,并利用时域有限差分算法探究该结构的光学特性。计算结果表明,当线性偏振光入射时,该结构表面激发出表面等离激元,且纳米孔间产生了局部表面等离子体共振,使得该结构的异常透射增强。针对这一现象,通过对中心孔与边孔所呈角度、入射光偏振角度、结构参数(中心孔直径、边孔直径、结构厚度、边孔与中心孔的间距)的调控来实现结构光学透射属性的优化。此外,分析所提结构在不同环境折射率条件下透射峰的变化规律,发现该结构也对周围的环境折射率具有较高的敏感度。因此该结构在表面等离激元滤波器和折射率传感器中具有广泛的应用前景。     

通断电自感综合演示实验

高三物理教材中的自感现象,大多是通过J2425型变压器原理说明器进行演示。有的学校可能没有,而且同用一件仪器,两次分别演示通电自感现象和断电自感现象,课堂上存在着操作麻烦的严重弊端,同时也不能给学生一个通断电自感的完整印象。为此,我对原演示实验进行了一些改进,不但能使通、断电自感现象一次完成,达到使用方便、印象完整的目的,而且还可观察断电后瞬时感生电流(电动势)的方向,有助于验证教材中所述“自感电动势总是阻碍导体中原来电流的变化的”这个结论。实验电路如图所示。     

Metamaterials and plasmonics: From nanoparticles to nanoantenna arrays,metasurfaces, and metamaterials

The rise of plasmonic metamaterials in recent years has unveiled the possibility of revolutionizing the entire field of optics and photonics, challenging well-established technological limitations and paving the way to innovations at an unprecedented level To capitalize the disruptive potential of this rising field of science and technology, it is important to be able to combine the richness of optical phenomena enabled by nanoplasmonics in order to realize metamaterial components, devices, and systems of increasing complexity. Here, we review a few recent research directions in the field of plasmonic metamaterials, which may foster further advancements in this research area. We will discuss the anomalous scattering features enabled by plasmonic nanoparticles and nanoclusters, and show how they may represent the fundamental building blocks of complex nanophotonic architectures. Building on these concepts, advanced components can be designed and operated, such as optical nanoantennas and nanoantenna arrays, which, in turn, may be at the basis of metasurface devices and complex systems. Following this path, from basic phenomena to advanced functionalities, the field of plasmonic metamaterials offers the promise of an important scientific and technological impact, with applications spanning from medical diagnostics to clean energy and information processing.     

The isolated critical value phenomenon in local－global riddling bifurcation

A chaotic synchronized system of two coupled skew tent maps is discussed in this paper. The locally and globally riddled basins of the chaotic synchronized attractor are studied. It is found that there is a novel phenomenon in the local－global riddling bifurcation of the attractive basin of the chaotic synchronized attractor in some specific coupling intervals. The coupling parameter corresponding to the locally riddled basin has a single value which is embedded in the coupling parameter interval corresponding to the globally riddled basin, just like a breakpoint. Also, there is no relation between this phenomenon and the form of the chaotic synchronized attractor. This phenomenon is found analytically. We also try to explain it in a physical sense. It may be that the chaotic synchronized attractor is in the critical state, as it is infinitely close to the boundary of its attractive basin. We conjecture that this isolated critical value phenomenon will be common in a system with a chaotic attractor in the critical state, in spite of the system being discrete or differential.