计算了相关态的振子强度和辐射跃迁率。
The oscillator strengths and radiation transition rates are also calculated.
计算了相关态的振子强度、跃迁几率和波长。
The oscillator strengths, transition rates and wavelengths are also calculated.
同时还计算了跃迁辐射波长、振子强度和跃迁率。
The wavelengths, oscillator strengths and radiation rates are also calculated.
价带顶和导带底附近的带间跃迁振子强度大部分都近乎为零；
Most optical oscillator strengths for the transitions between valence band and conduction band are nearly equal to zero.
因此可以定义每单位激发能内的广义振子强度为广义振子强度密度。
Thus, we can define the generalized oscillator strength density as the strength per unit excitation energy.
利用该装置测量了一氧化碳分子的光电离效率曲线及其离子碎片的部分光学振子强度密度。
The photoionization efficiency curve and the partial optical oscillator strength densities for different fragments of CO was determined by this work.
讨论了氯化铯型离子晶体束缚激子的结合能、极化波振子强度、零色散波长和微观参数之间的关系。
The strengths of the polarization wave oscillator are calculated. The material dispersion and the zero dispersion wavelengths f…
计算量子点分子中束缚能级之间跃迁的振子强度表明，只有成键态和相应的反键态之间跃迁才是允许的。
And the bound state with the highest energy level in the quantum-dot molecule changes gradually into a quasibound state when the electric field strength increases.
为了统一处理束缚态到束缚态和束缚态到连续态的跃迁，根据量子数亏损理论定义了广义振子强度密度。
In order to treat the bound-bound and bound-continuum transitions in a unified manner, the generalized oscillator strength density is defined.
计算结果表明，采用二体关联波函数计算振子强度不仅简便省时，而且精度与远为复杂的CI方法相近。
The calculated results show that this kind of calculation method is not only very simple and time-saving but with high accuracy which is equivalent to those obtained by CI method.
在PM3/CIS水平上计算了它们的电子光谱，得到了由基态到各激发态的垂直跃迁能和相应的振子强度。
At PM3/CIS level, the vertical excitation spectra were calculated and the vertical excitation energies and corresponding oscillator strength from the ground states to the excited states are obtained.
在PM3/CIS水平上计算了它们的电子光谱，得到了由基态到各激发态的垂直跃迁能和相应的振子强度。
At PM3/CIS level, the vertical excitation spectra were calculated and the vertical excitation energies and corresponding oscillator strength from the ground states to the excited states are obtained.
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