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oscillator wave function 振子波函数
The expression for radial wave function of a two dimensional harmonic oscillator is derived through an integral formula of general Lagurre function. 利用广义拉盖尔函数的一个积分公式,推导出二维各向同性谐振子的归一化径向波函数表达式。
From the generalized linear quantum transformation theory,we obtain the normal product form of evolution operator and the wave function for a time-dependent oscillator. 由广义线性量子变换理论，得到了含时谐振子正规乘积形式的演化算符和波函数的严格表达式.
The molecular electronic wave function is perturbed. 分子的电子波函数受到了微扰。
We now show how to calculate molecular dipole moments from wave function. 我们现在说明如何从波函数来计算分子的偶极矩。
The ground state energy and the wave function of a linear harmonic oscillator are solved by Euler equation comforted to functional extremum. 利用泛函极值满足的Euler方程 ;解出了线性谐振子的基态能量和波函数 .
By using some formulae of confluent hyper-geometric function, the results of radial operators on the normalizing radial wave function of a 3-D isotropic harmonic oscillator are derived, and the ladder operators are given to calculate the matrix elements. 摘要利用合流超几何函数的递推关系式得到径向算符对归一化径向函数的作用结果，得出其升降算符通项，便于求解矩阵元。
If so we shall have a wave function that satisfies our new postulate. 如果事实确是如此，我们就得到了一个满足新假设的波函数。
If so we shall have a wave function that satisfies our new postulate . 如果事实确是如此，我们就得到了一个满足新假设的波函数。
These wave functions correspond to states of constant energy E. 这些波函数对应于具有恒定能量E的态。
The angular part of a continuum wave function is, of course, a spherical harmonic. 连续谱波函数的角度部分当然是球谐函数。
These wave functions correspond to states of constant energy E . 这些波函数对应于具有恒定能量e的态。
In the quantum world, objects are described by wave functions. 在量子的世界中，物体都是以波函数来描述。
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。
The decay oscillating wave pulses can be applied in situations such as demagnetization of permanent magnets. 交流衰减波电流可用于永磁体的退磁等应用中。
Wave function, Schrodingger equation, infinite deep potential well in one dimension. 波函数;薛定谔方程;一维无限深势阱;
Let's have a look at an interesting feature of the ground-state wave function, Eq(6. 120). 让我们来看基态函数(6.;120)式的有趣图象。
We start by considering the wave function, ignoring the antisymmetry requirement. 我们先考虑波函数,而暂不顾及它的反对称性要求。
If desired, the perturbed wave function may be normalized at the end of the calculation. 当需要时，可在计算最后将微拢波函数归一化。
Although the approximate wave function is qualitatively useful, it is gravely lacking in quantitative accuracy. 虽然近似的波函数是定性地有用，然而它严重的缺少定量的准确性。