能级劈裂

在一定条件下能级劈裂有利于原子偶级压缩的产生。

Atomic energy level splitting is helpful to dipole squeezing generation under certain conditions .

在此基础上，对高Z元素高离化度离子的能级劈裂规律进行仔细分析，建立了计算高Z高剥离态离子相对论组态平均能的解析拟合公式。

According to this method , the regular changes of the energy splitting occurred in highly-charged ions are carefully studied , and analytically fitted formulas for calculating the subconfiguration-averaged energies of high Z elments are given .

缺陷的四极能级劈裂和双共振的过程在文中进行了分析。

Quadrupole splittings of the imperfections and the double-resonance process are analyzed in this paper .

结果表明：对于异自旋三自由基体系，形成异自旋后对称性降低使部分占据的近简并轨道能级劈裂值增大，反铁磁耦合作用普遍增强。

Th e result shows that part-occupied near-degenerate orbitals split value and dia ferromagnetic coupling increases when symmetry of hetero tri-radicals decreases .

介绍了与磁性电极耦合的量子点的近藤共振、单电子能级自旋劈裂、磁化和线性电导等物理性质。

The properties of a quantum dot coupled with two magnetic electrodes , such as the Kondo resonance , spin-splitting of single electron levels , magnetization , and linear conductance , are discussed .

测量了玻璃中Er~（3+）的1.5μm近红外发射的变温光谱，利用简化模型得到了Er~（3+）的~4I（13／2）能级高能Stark劈裂态的光谱。

1.5 μ rn emission spectra of the Er3 + - doped glasses at different temperatures were measured , and the spectra of high-level Stark sublevel of 4I_ ( 13 / 2 ) level were obtained using a simplified model .

磁场的作用是产生能级的塞曼劈裂和调控超精细相互作用。

The role of the magnetic field is to produce the split of the energy level and to regulate the hyperfine interaction .

而近藤共振和单电子能级的自旋劈裂都可以通过电极的内部磁化强度来控制，可以用来产生自旋阀效应。

Both the Kondo resonance and the spin-splitting of the single electron levels can be controlled by internal magnetization of the electrodes , which can be used to generate a spin-valve effect .

并且通过计算自旋-轨道相互作用以及自旋-其他轨道相互作用算符的期待值得到能级的精细结构劈裂。

The fine structures are determined by computing the expectation values of the spin-orbit and spin-other orbit interaction operators .

由辐射谱发现，在强、中耦合区上能级将发生不同的劈裂；在弱耦合区，腔衰减率控制原子的自发辐射性质，上能级不发生劈裂。

It is shown that in strong and intermediate coupling regime , the upper level splits in different ways . In weak coupling regime , the atomic spontaneous emission properties were determined by the cavity decay rate , and the upper level does not split .