1) Hubbard operators
Hubbard算符
1.
Aiming at the transformation of Hamiltonian from Pauli matrices to Hubbard operators, the authors use the unity and orthogonal of Hubbard operators to give the transforming formula of Pauli matrices and Hubbard operators, by which, they realize the change from Pauli matrices to Hubbard operators.
把用Pauli算符表示的哈密顿量转化成用Hubbard算符表示。
2.
Aim The Hamiltonian is transformed from Pauli matrices to Hubbard operators.
目的把用Pauli矩阵表示的哈密顿量转化成用Hubbard算符表示。
3.
We use the unity and orthogonal of Hubbard operators to give the transforming formula of Pauli operators and Hubbard operators,by using these transforming formula we realize the change from Pauli operators to Hubbard operators.
文章以各向异性自旋梯模型的哈密顿量作为例子,利用Hubbard算符的归一性和正交性给出了Hubbard算符和Pauli算符之间转化的运算公式,从而把用Pauli算符表示的各向异性自旋梯模型的哈密顿量转化成用Hubbard算符表示。
2) operator
[英]['ɔpəreɪtə(r)] [美]['ɑpə'retɚ]
算符
1.
Discussion on the existence of common eigenstates for any two operators;
对一般算符是否存在共同本征态问题的讨论
2.
On Some Kinds of Operator Operation Methods in Quantum Mechanics;
浅谈量子力学中算符运算的多种求法
3.
The operator theory method lead to the uncertainty relation of one dimensional infinite well;
一维无限深势阱不确定关系的算符理论推导法
3) operator aN
算符aN
1.
The characteristics of the k th-power squeezing of a class of superposition states which involving two orthonormalized eigenstates of photon annihilation operator aN are studied.
对一类光子消灭算符aN的正交归一本征态的迭加态的振幅k次方压缩特性进行研究,结果表明一类aN的正交归一本征态的迭加态的振幅k次方压缩特性明显地区别于aN的正交归一本征态k次方压缩。
4) arithmetic operator
算术算符
5) operator-symbol
运算符符号
6) The operator O is the null operator.
算符O是零算符。
补充资料：Γ算符
分子式：
CAS号：
性质： 或称Γ算符，其定义为：。即它是右矢|ψ>与左矢<ψ|的乘符号。若用波函数来表示，则密度矩阵可表示为：应用密度矩阵概念可把求力学量算符G平均值的积分问题简化为简单的代数问题，因G与г算符的乘积的迹即其平均值<G>=<ψ|G|ψ>=TrGΓ。
CAS号：
性质： 或称Γ算符，其定义为：。即它是右矢|ψ>与左矢<ψ|的乘符号。若用波函数来表示，则密度矩阵可表示为：应用密度矩阵概念可把求力学量算符G平均值的积分问题简化为简单的代数问题，因G与г算符的乘积的迹即其平均值<G>=<ψ|G|ψ>=TrGΓ。
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