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1)  optical dipole potential
光学偶极势
1.
We calculate the corresponding intensity distribution,the optical dipole potential and its dipole force for 23Na atoms.
计算了漏斗的光强分布及其光学偶极势与偶极力分布。
2)  optical dipole trap
光学偶极阱
1.
Based on our present experimental system,we propose a scheme of generating adjustable multiple optical dipole traps by using three strongly focused beams,which implies controllable optical lattice for atom manipulation.
本文基于目前的实验系统,提出了利用由三组驻波场组成的强聚焦光学系统产生间距可控的光学晶格,并在此基础上实现多光学偶极阱的一种方案。
3)  dipole-like warming trend
偶极子增暖趋势
4)  laser dipole force
激光偶极力
5)  Optical potential
光学势
1.
The dispersion relation is included into the optical potential.
在光学势中引入色散关系,相比于通常的耦合道光学模型,极大地减少了光学势参数的个数。
2.
The differential cross sections and the spin observables of p- ~ 12 C elastic scattering in the whole intermediate energy region are calculated using the KMT multiple scattering theory with microscopic momentum space optical potential which incorporates the spin dependence of the NN and p- ~ 12 C interactions.
在KMT理论框架下,应用微观的动量空间一级光学势,包括了库仑修正,自旋关联,NN振幅反对称,离壳效应,核子反冲和结合能转换,Lorentz不变的角变换。
3.
From the framework of the multiple scattering theory, we obtain the antiproton-nucleus optical potential that can best describe the experimental elastic scattering data.
从多次散射的理论框架,获得反质子的光学势,这一光学势能很好地描述从轻核至重核在整个能区的弹性散射实验。
6)  deep optical
深光学势
1.
The results show that the double-alpha transfer effect for a deep optical potential is responsible for the above difference in the elastic scattering excitation functions between these two systems.
基于核分子轨道理论分析了20Ne+12C系统所展示的基本特征,并且再现了该系统弹性散射激发函数和角分布,研究结果表明,使用一个深光学势的双α转移效应,是产生这两个系统弹性散射激发函数之间差别的重要原因。
补充资料:极势
1.使势力丧尽。
说明:补充资料仅用于学习参考,请勿用于其它任何用途。
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