Irreducible representation
- 不可约表示
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The Base Function of the Irreducible Representation for Point Groups in the Expansion of Free Energy
自由能展开式中点群的不可约表示的基函数
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The calculation of characters of group representation is the basis of studying the irreducible representation of groups .
计算各种群的特征标,是研究群不可约表示的基础。
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The Method of Configuration Interaction of Irreducible Representation Basis Functions of Symplectic Chain
辛群群链不可约表示基函数的组态相互作用方法
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Irreducible representation of the odd - degree complex Clifford algebra
奇数次复Clifford代数的不可约表示
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Comparison of Calculation Methods and Application of Circularity Molecule ( CH ) _n Irreducible Representation Radix
对环状(CH)n分子不可约表示的基的计算方法比较与应用
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Many of the important applications of complex Clifford algebra come from the irreducible representation of complex Clifford algebra .
有关复Clifford代数的许多重要应用来源于复Clifford代数的不可约表示。
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For the molecular orbital , the irreducible representation component is analyzed besides the membership function of the fuzzy symmetry transformation .
对于分子轨道,除模糊对称变换的隶属函数外,分析了所属不可约表示成分。
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The Irreducible Representation of the Numberator point Group
分子点群的不可约表示
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Clebsch-Gordan Coefficients of Space Groups and the Method of Disposition of the Phase Factor in the Process of Computation by the Irreducible Representation
关于空间群的C&G系数及IR表示的计算中位相因子的处理方法
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It is easy to prove that the irreducible representation of finite group satisfies orthogonal relation through the usage of Schur Lemma .
利用舒尔引理,很容易证明有限群的不可约表示满足正交关系。
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The total antisymmetric basis functions are constructed for irreducible representation of S3 permutation group from nine-dimensional hyperspherical harmonics .
以九维超球谐为投影函数,构造置换群S3一维不可约表示的全反称基函数。
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In the paper We present a Calculating method for eigenvalue of CSCO-I of Ih group using Table of characters of irreducible representation of Ih group .
本文提供一种由Ih群的不可约表示的特征标来求Ih群的CSCO-I本征值谱的方法。
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By using two different methods , we acquire irreducible representation radix of circularity molecule . If we reasonably use the symmetry of system , it is convenient to calculation course .
利用体系的对称性,用两种不同方法求出对环状(CH)n分子的不可约表示的基,大大地简化了计算。
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The laws of physics has its group , The class of irreducible representation of group decides the structure of the system of quantum , such as H2O electronic eigenstate .
物理规律对应着确定的群,群的不可约表示对H空间的态矢分类可方便地决定一个量子系统的结构。并对H2O的电子态进行了分析。
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The calculated results are classified according to irreducible representation of molecular point-group , and it is thus convenient to analyze data by means of group theory and correlate with experimental spectroscopic dade , etc.
计算结果按分子点群不可约表示分类,便于从群论的观点讨论分子能谱并与实验数据进行对比。
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In the frame of irreducible representation of Poincar é group , this spin operator , which is named as moving spin and applied to all the canonical states of the particle , is constructed .
在Poincar啨群不可约表示的框架里,构造了适用于粒子任意正则态的自旋算符,称为运动自旋。
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In this paper , we calculate the irreducible representation of magnetic space group by using the co-representation theory of magnetic group and calculate the C-G coefficients of the structure for magnetic space group by eigenfunction method ( EFM ) .
本文利用磁群共表示理论构造出磁空间群的不可约表示,进而利用本征函数法计算了O10h结构磁空间群的CG系数。
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The generators and irreducible representation coherent state of the SU ( 2 ) group are constructed using the inverse operators of bose harmonic oscillator . The inhomogeneous inverse differential realizations of the SU ( 2 ) group are derived .
利用玻色振子的逆算符构造了SU(2)群的生成元和不可约表示的相干态,进而导出了SU(2)群的非齐次逆微分实现。
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The bonding properties are analysed . The relation between the H-F force and the MO 's irreducible representation is presented , a method to decide the molecular geometric configuration variation of excited states by the frontier MO 's H-F force is suggested .
用从头算法计算了乙烯和环丙烷的各分子轨道的H-F力,指出了H-F力与分子轨道不可约表示闻的关系,提出了用前线轨道的H-F力判断激发态分子构型畸变的方法。
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By using the inverse matrix of Cartan matrix , the expansion of the highest weight of any irreducible representation for the simple Lie algebra g by its simple roots is given , and the expression of given by Dynkin for the simple Lie algebra is also obtained .
利用Cartan矩阵的逆矩阵,得到了单李代数g任一不可约表示的最高权关于g的素根的展开式,并得到了Dynkin所给的单李代数r值的表达式。