共查询到20条相似文献,搜索用时 134 毫秒
1.
一、引 言 电子通道效应是扫描电镜中的一项重要物理现象,它的发现进一步扩大了扫描电镜在材料科学和金属物理中的应用. 对电子与晶体相互作用的研究表明,入射电子被晶体的散射几率是同它相对于(hkl)晶面的入射角有关.在某些入射方向下,电子被散射的几率较大(相当于禁道),而在另一些入射方向下,电子被散射的几率较小(相当于通道),这种现象称为电子通道效应. 在扫描电镜中,应用电子通道效应所产生的花样和显微象称为电子通道花样和通道显微象.由于上述花样和显微象能反映晶体的位向、晶体的表面状态以及晶体的不完整性,因此,它在材料科学和金… 相似文献
2.
在扫描电镜中,应用电子通道效应所产生的花样称为电子通道花样(简写为ECP).作为ECP的应用和分析基础,首先必须对ECP进行几何测量和结晶学注释.本文作为1982年第11卷第12期《物理》讲座栏内“电子通道效应及其应用”[1]一文在实验方法上的补充,以便对这个专门的问题进行系统的阐述. 一、ECP的成象几何关系 在文献[1]中曾系统地阐述了ECP的成象几何关系的特点.根据这些特点,并引入等效投射距离R这个参数,则可以画出ECP的成象等效几何关系,如图1所示. 在图1中,两个相交的电子通道带依次属于(hikili)晶面和(hikili)晶面,这两个晶面的晶… 相似文献
3.
4.
5.
6.
7.
本文探索波驱动等离子体电流的一种新机制,称之为随机驱动效应。在相干波与磁化等离子体相互作用的系统中,当波的强度超过某个阈值时,速度空间中的一些共振区将互相重迭。共振区的重迭可导致粒子的随机运动,引起速度空间中的扩散现象。如果在电子平行于磁场方向的速度分布中,这种重迭区是不对称的,这样,就可驱动纵向等离子体电流。
关键词: 相似文献
8.
化学诱导动态核极化(Chemically Induced Dynamic Nuclear Polarization,简称CIDNP)是一种在化学反应体系中观察到的NMR谱线强度反常的现象(常称之为极化谱,包括增强吸收和发射等)。1967年由Bargon和Fischer[1] (西德)以及Ward和Lawler[2] (美国)首先发现的。由于他们所研究的反应体系中涉及自由基,因此最初认为这种谱线强度反常现象是由于自由基中间体中的电子-核交叉弛豫引起的。这种机理通常称为:Overhauser型的动态核极化(Dynamic Nnclear Polarization简称DNP)。但很快就发现它不足以解释实验得到的结果,而CIDNP的命名却是这样因袭下来了。 相似文献
9.
10.
在掺Si的GaAs/AlGaAs二维电子气(2DEG)结构中,得到μ2K=1.78×106cm2/(V·s)的高迁移率.在低温(2K)和高磁场(6T)的条件下,对样品进行红 光辐照,观察到持久光电导(PPC)效应,电子浓度在光照后显著增加.通过整数量子霍尔效应 (IQHE)和Shubnikov-de Haas (SdH)振荡的测量,研究了2DEG的子带电子特性.样品在低温光 照后2DEG中第一子带和第二子带的电子浓度同时随电子总浓度的增加而增加;而且电子迁移 率也明显提高.同时,通过整数霍尔平台的宽度对光照前后电子的量子寿命变短现象作了理 论分析.
关键词:
二维电子气
量子霍尔效应
SdH振荡
持久光电导效应 相似文献
11.
S. Friedrichs R. R. Meyer J. Sloan A. I. Kirkland J. L. Hutchison M. L. H. Green 《Physics of the Solid State》2002,44(3):463-466
The detailed inclusion crystallography of a one-dimensional valentinite Sb2O3 crystal incorporated within a helical (21, ?8) single-walled carbon nanotube (SWNT) was identified from a phase image that was recovered via a modified object wave restoration scheme. A detailed analysis of asymmetric fringe contrast in the tube walls provided strong evidence for the chiral sense of the tube itself. Due to the good agreement of the observed wall periodicity with the determined absolute focus values and power spectra obtained from single-pixel line traces along both tube walls, we were able to determine the chiral sense of the SWNT and the tilt angle of the Sb2O3/SWNT composite relative to the electron beam. The angle between the optimum $\left\langle {10\bar 1} \right\rangle $ viewing direction of the crystal fraction and the tube axis, which is aligned with the $\left\langle {4\bar 12} \right\rangle $ direction of the Sb2O3 crystal, is 78.3°. Since small deviations from this viewing direction make an insignificant difference to the observed contrast, a tube inclination of 15° is plausible for both the Sb2O3 crystal and the assigned (21, ?8) SWNT, which is the mirror image of a (13, 8) SWNT. 相似文献
12.
Dinesh Pathak R. K. Bedi Davinder Kaur 《Applied Physics A: Materials Science & Processing》2009,95(3):843-847
AgInSe2 films were prepared by a thermal evaporation technique onto Si(100) substrates at a pressure of 10−5 mbar. Structural and optical properties of films deposited at 300 and 473 K have been investigated. The film composition
was studied by energy dispersive analysis through X-rays. X-ray diffraction patterns indicate that AgInSe2 films have chalcopyrite structure with strong preferred orientation in the (112) direction. Average vertical crystallite
size of 25 nm was observed. The optical energy gaps of 1.20 and 1.90 eV were obtained due to the fundamental absorption edge
and a transition originating from crystal field splitting, respectively. Field emission scanning electron microscopy shows
loosely packed grains of spherical symmetry with some facets. 相似文献
13.
14.
The branched crystal morphology of linear polyethylene formed at various temperatures from thin films has been studied by
atomic-force microscopy (AFM), transmission electron microscopy (TEM), electron diffraction (ED) pattern and polymer decoration
technique. Two types of branched patterns, i.e. dendrite and seaweed patterns, have been visualized. The fractal dimension d
f = 1.65 of both dendrite and some of seaweed patterns was obtained by using the box-counting method, although most of the
seaweed patterns are compact. Selected-area ED patterns indicate that the fold stems tilt about 34.5° around the b-axis and polymer decoration patterns show that the chain folding direction and regularity in two (200) regions are quite
different from each other. Because of chain tilting, branched crystals show three striking features: 1) the lamella-like branches
show two (200) regions with different thickness; 2) the crystals usually bend towards the thin region; 3) the thick region
grows faster by developing branches, thus branches usually occur outside the thick region. The branched patterns show a characteristic
width w, which gives a linear relationship with the crystallization temperature on a semilogarithmic plot.
Received 15 March 2002 and Received in final form 29 April 2002 相似文献
15.
The morphology and orientation of multi-ferroic β′-(Sm,Gd)2(MoO4)3 crystals in the lines patterned by laser irradiations in 3Sm2O3–18.25Gd2O3–63.75MoO3–15B2O3 (mol%) glass were examined using transmission electron microscope (TEM) observations in order to clarify the origin of the appearance of periodic birefringence in an atomic-scale level. The crystallographic direction of crystals in the lines was determined from selected area electron diffraction (SAED) patterns in TEM observations, and it was demonstrated that a gradual rotation of crystallographic axes takes place along the crystal growth direction (laser scanning direction). The unique crystal growth with a spiral-like rotation of the crystallographic axes is due to the gradual rotation of (MoO4)2− tetrahedral units in β′-(Sm,Gd)2(MoO4)3 crystals. The laser-induced crystallization, in which the region and direction of crystal growth are restricted artificially to a narrow space, provides a new crystal growth engineering. 相似文献
16.
本文利用透射电子显微相和电子衍射相对18Ni马氏体时效钢中沉淀强化相和时效结构的结晶学性质进行了研究。利用数个不同晶带的衍射相,一致地鉴别出同时存在Ni3Mo,Ni3Ti沉淀相和弥散的逆转变奥氏体,并且确定了它们相对马氏体基体的取向关系。证明了沉淀相、逆转变奥氏体与基体之间,密排面和密排方向都相互平行。指出在透射电子显微相中看到的魏氏型沉淀结构,实际上是由棒状沉淀相构成的三维空间格条结构,其中棒状沉淀相的长度方向平行于基体的四个〈111〉型方向。所观察到的扩张位错和位错塞积的真实性需要更多的实验证实。从结构观点,讨论了沿位错线的沉淀过程,并提出了钴钼交互作用的可能机制。 相似文献
17.
The Compton profiles of orthorhombic sulphur crystals have been measured the scattering vector perpendicular to the crystal planes (110) and (001) using 60 keV radiation from a 241Am source. Significant anisotropy was observed in the electron momentum distribution. Fourier transformed Compton profiles were compared with theoretical autocorrelation functions for a S8 ring molecule. It is shown that the observed anisotropy can be only partially interpreted in terms of intermolecular interactions. The strong correlation, observed in the direction perpendicular to the plane of the S8 ring indicates a meaningful ring — ring interaction in the orthorhombic sulphur crystal. 相似文献
18.
Yin-Sheng Peng Bo Xu Xiao-Ling Ye Jie-Bin Niu Rui Jia Zhan-Guo Wang 《Optical and Quantum Electronics》2009,41(3):151-158
This work discusses the fabrication of two-dimensional photonic crystal mask layer patterns. Photonic crystal patterns having
holes with smooth and straight sidewalls are achieved by optimizing electron beam exposure doses during electron beam lithography
process. Thereafter, to precisely transfer the patterns from the beam resist to the SiO2 mask layer, we developed a pulse-time etching method and optimize various reaction ion etching conditions. Results show that
we can obtain high quality two-dimensional photonic crystal mask layer patterns. 相似文献
19.
飞秒激光聚焦到LiF晶体内部, 晶体的加工形貌随偏振改变. 实验表明, 偏振方向平行于<110> 晶向时, 加工起点到表面的距离是<100>偏振下的1.08 倍; 而<110>偏振下加工终点到表面的距离是<100> 偏振下的1.01 倍. 为了解释加工形貌的偏振依赖, 建立了逆韧致辐射、雪崩电离和无辐射跃迁的模型, 首先, 价带电子通过强场电离和雪崩电离, 从激光中吸收能量跃迁到导带, 该过程用电子密度演化方程和傍轴非线性薛定谔方程描述, 求解方程得到导带电子密度; 其次, 导带电子通过无辐射跃迁过程释放能量给晶格, 由能量守恒计算出晶格温度沿激光传播方向的分布; 最后, 晶格温度超过熔点以上的区域被加工. 模拟结果显示, <110>偏振下加工起点到表面的距离是<100> 偏振下的1.03倍, 而<110>偏振下加工终点到表面的距离是<100>偏振下的0.981 倍, 与实验结果基本一致. 虽然Z扫描技术测量的非线性折射率随偏振方向变化, 但是非线性折射率的变化趋势与实验结果相反. 模拟和实验证明逆韧致辐射导致加工形貌随偏振变化. 相似文献
20.
本文采用分子动力学方法研究了沿<100>及<111>晶向的单轴应变对钨中单个氦原子扩散的影响。结果表明,应变会使得金属钨材料发生相变,且引起相变的临界应变随温度升高而减小。相变起始的应变在达到抗拉强度的应变附近。计算结果表明,拉应变使得单个氦原子在钨中的扩散系数发生骤降,在不同应变下扩散系数变化平缓。沿<100>晶向氦扩散系数随应变的增大而线性减小,而<111>晶向则出现了震荡变化趋势。研究结果表明,沿<100>晶向应变达到+0.15%时阿纽列斯方程不再适用,而沿<111>晶向应变大+5%阿纽列斯方程仍然适用;沿<111>晶向随应变增加氦扩散激活能减小,说明应变使得单个氦原子在钨中迁移性增强。 相似文献