1) rotor-stator interaction
子域干涉
1.
Partitioning algorithm for N-S equations in relative/absolute cylindrical-coordinate systems and investigation on treatment for rotor-stator interaction;
动静圆柱坐标系下N-S方程的分区算法及子域干涉处理研究
2) localized interference
定域干涉
1.
This paper deduces a general use formula on the optical path of difference under various circumstance concerning localized interference of A.
该文推导出迈克尔孙干涉仪定域干涉各种情况下光程差的通用公式,通过实验对光波波长的测定进行讨论,并在此基础上提出了进一步提高光波波长测定精度的有效途径。
2.
It is put forward that the localized and non-localized interference are produced by different light source separately,and the interference of equal thickness or of equal inclination depends on the angle between M_1 and M′_2 and the thickness d inside them.
对物理实验迈克尔逊干涉仪的调节和使用中常存在的几个问题进行分析和讨论,指出形成定域或非定域干涉取决于光源,产生等倾或等厚干涉不仅与M1与M′2之间的夹角α有关,还受其间的空气层厚度d影响。
3) interference area
干涉区域
4) Quantum interference
量子干涉
1.
Effect of vacuum-induced coherence in a four-level atomic system via quantum interference;
基于量子干涉效应的四能级原子系统中的vacuum-induced coherence效应
2.
Quantum interference induced by two lasers in potassium;
双色场中钾原子的量子干涉现象
3.
Two-photon resonant nondegenerate four-wave mixing via quantum interference;
引入量子干涉的双光子共振非简并四波混频
5) electron interference
电子干涉
1.
The calculated position of peak of photocurrent on the basis of theory of electron interference is in very good agreement with the experimental results.
2 9μm附近存在一个强电流峰 ,分析认为 ,该电流峰与多量子阱势垒以上的电子干涉有关 。
2.
On the basis of theory of electron interference, it is pointed out that there are a series of separate weak interference non-localized states above barrier for multiquantum well.
根据电子干涉理论分析指出 :多量子阱结构势垒以上的电子 ,由于其干涉效应形成一些分立的弱干涉非定域态。
6) atomic interference
原子干涉
1.
A scheme for the generation of superpositions of squeezed coherent state based on the atomic interference is presented.
在文中我们提出了一种基于原子干涉的方法产生压缩相干迭加态。
补充资料：超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
超导电性的局域和非局域理论（localizedandnon-localizedtheoriesofsuperconductivity）
伦敦第二个方程（见“伦敦规范”）表明，在伦敦理论中实际上假定了js(r)是正比于同一位置r的矢势A(r)，而与其他位置的A无牵连；换言之，局域的A(r)可确定该局域的js(r)，反之亦然，即理论具有局域性，所以伦敦理论是一种超导电性的局域理论。若r周围r'位置的A(r')与j(r)有牵连而影响j(r)的改变，则A(r)就为非局域性质的。由于`\nabla\timesbb{A}=\mu_0bb{H}`，所以也可以说磁场强度H是非局域性的。为此，超导电性需由非局域性理论来描绘，称超导电性的非局域理论。皮帕德非局域理论就是典型的超导电性非局域唯象理论。
说明：补充资料仅用于学习参考，请勿用于其它任何用途。
参考词条