说明:双击或选中下面任意单词,将显示该词的音标、读音、翻译等;选中中文或多个词,将显示翻译。
您的位置:首页 -> 词典 -> 正则动量算符
1)  canonical momentum operators
正则动量算符
2)  normal operators
正则算符
3)  momentum operator
动量算符
1.
Discussion on a relativity momentum operator;
一个相对论性动量算符公式的再讨论
2.
This article discusses in detail about the presentation of the momentum operator P under coordinate representation.
对坐标表象中动量算符声的具体表示进行了讨论。
3.
It is proved that the components of relativitic momentum operator in any coordinate,in-cluding the curve coordinate,is compoment operator of momentum,and it is impossible that there exist the term relative to spin matrix.
指出相对论性动量算符p^在任何坐标系中的分量 ,包括在曲线坐标系中的分量也是动量分量的算符 ,不可能出现与自旋矩阵有关的项 。
4)  canonical momentum
正则动量
5)  momentum operator P^
动量算符^P
6)  angular momentum operator
角动量算符
1.
This paper begins with the commutation relation of abstract angular momentum operator, and then utilizes the corresponding raising operator and the lower operator to directly solve the eigenvalue and the same eigenvector of J2 and Jz.
从抽象的角动量算符的对易子关系出发,利用相应的上升算符和下降算符,直接求解J2和Jz的本征值和共同本征矢,在坐标基中得到轨道角动量算符L2和Lz的共同本征函数。
2.
Previous results related to the appropriate spin operator and the angular momentum operator for a relativistic particle with arbitrary spin and nonzero mass are discussed in an alternative way.
在动量表象下对非零质量带自旋粒子的角动量算符和推动矢量算符也即Lorentz变换生成元进行了讨论 ,得到了它们按轨道和自旋两部分分拆的新的表达
3.
It is pointed out that the angular momentum operator J ^ does not have complete set of eigenvalues and eigenvectors,the dynamical quantity described by angular momentum operator J ^ is non observable,it is not appropriate to treate angular momentum J as a whole.
指出了角动量算符J ^不存在本征值和本征矢量完全集 ,角动量算符J ^不描写一个可观察量以及角动量J不宜作为整体来讨论 。
补充资料:风胜则动

风胜则动

风胜则动   病因病理学术语。出《素问·阴阳应象大论》。风气偏胜则病症表现摇动性或游走多变的特点。如游走性的关节肌肉疼痛、眩晕、震颤、四肢抽搐、角弓反张、口眼斜、卒然昏仆等。

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