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1.
In fact, we could make the substitution and still wind up with the correct eigenfunctions and eigenvalues.
事实上,我们可以做这种代换而仍能绕弯得出正确的本征函数和本征值
2.
The procedure described above applies to the eigenvalues and eigenfunctions of any Hermitian operator.
用上述运算方法也能求出任一厄密算符的本征值和本征函数。
3.
Quantum invariant eigenvalue and eigen function of quantum invariant operator of time-dependent damped harmonic oscilator;
含时阻尼谐振子的量子不变量算符及其本征值和本征函数
4.
Calculation of energy characteristic value and characteristic function of hydrogen atoms with a kind of calculating signs;
用一种算符计算氢原子的能量本征值和本征函数
5.
The Solutions of eigenvalue and eigenfunction for three non-self-adjont situation are summrized.
对三种非自共轭情形下的本征值和本征函数的求解方法进行了归纳总结。
6.
Since we get continuous rather than discrete allowed values for E≥0, the positive-energy eigenfunctions are called continuum eigenfunction.
由于对E≥0得到连续的而非分立的允许值,正能量的本征函数叫做连续谱本征函数。
7.
If only the eigenvalue of A and not the eigenfunctions are desired, it is not necessary, according to Section 3. 3, to obtain the transformation matrix S.
假如仅需求出A的本征值而不要求出本征函数,那么按照本章第3.3节,就不必求出变换矩阵S。
8.
Abstract: The wavefunctions and energy eigenvalues for the ring-shaped oscillator are obtained using the ideas of supersymmetric quantum mechanics and shape invaricace.
文摘:采用量子力学中的超对称性和形不变性,讨论环形振子的波函数和能量本征值.
9.
Dual Relation between Production Function and Cost Function;
生产函数与成本函数的对偶关系及其特征
10.
Computation of Energy Levels of I_2 Molecule by Spherical Bessel Function Expansion Method
I_2分子振动本征函数的球贝塞尔函数展开法
11.
The Stability of Bénard System and the Orthogonality of Eigenfunction;
Bénard系统的稳定性与本征函数的正交性
12.
EIGENFUNCTION METHOD FOR A GENERALIZATION OF BLACK-SCHOLES;
推广的Black-scholes模型的本征函数解法
13.
Wigner Functions for Eigenstates of Arbitrary Power of Annihilation Operators
湮灭算符任意次幂本征态的Wigner函数
14.
The paper presents a model of turbulent flow, which can exactly provide data of the characteristic length and velocity of turbulent flow.
本文介绍的紊流模型能准确提供特征速度和特征长度参数的数值。
15.
maximum characteristic root
特征函数根的极大值
16.
Eigen-values and Eigen-wavefunctions of the Bound Electronic States in a Finite Semi-parabolic Quantum Well;
有限深半抛物量子阱中束缚电子态的本征能量与本征函数
17.
The parity of the eigenfunction is found by determining what happens to the wave function when r is replaced by -r.
本征函数的宇称可以这样确定:当r用-r代替时看波函数的变化。
18.
The value of the stationary states but also the corresponding functions ψ(orψ=ψe????), the so-called eigenfunctions.
并且还给出相应的函数ψ(ψ=ψe????),这就是所谓的本征函数。