Hg的Zeeman效应相对强度实验观察与朗德g因子测量

利用气压扫描式Fabry-Perot标准具测量置于磁场中Hg原子激发态的塞曼光谱,观察谱线404.66 nm,435.83 nm,546.07 nm,579.07 nm的Zeeman分裂,定量测定了各谱线的相对强度,并由此得到各能级的朗德g因子.     

Rashba效应和Zeeman效应对各向异性量子点中束缚磁极化子性质的影响

采用Pekar变分法和幺正变换相结合的方法研究了各向异性量子点中束缚磁极化子的Rashba效应和Zeeman效应.通过理论推导,得到束缚磁极化子基态能量的表达式.讨论了极化子基态能量与横向有效受限长度、纵向有效受限长度、磁场回旋共振频率、库仑束缚势的关系.由于晶体结构反演非对称性和时间反演非对称性,极化子能量发生Rashba自旋轨道分裂和Zeeman分裂.在强、弱磁场下,分别讨论了Zeeman效应和Rashba效应在能量分裂中所占的主导地位.由于声子和杂质的存在,极化子比裸电子态更稳定.     

Zeeman效应实验一定能推断出原子的g_J值吗?

本文以实例对Zeeman效应一定能推断原子的gJ值问题做了否定的回答。     

J＇K耦合的Zeeman效应

在分析光谱数据基础上，本文以Ｎｅ原子６３２８谱线为Ｊ’Ｋ耦合Ｚｅｅｍａｎ效应实例计算了谱线在较弱磁场中的分裂情况；从而廓清了有关教材中不正确的论述。     

原子光谱中同位素位移和超精细结构分裂

利用共线快离子束-激光光谱学方法测量了钕离子所有7个稳定同位素(A=142～146,148,150)之间的同位素位移和两个奇同位素(A=143,145)的超精细结构分裂．     

Ba原子6s5d~3 D与6p5d~3 F态的超精细结构及态间跃迁的同位素移动的直接确定

提出并演示了一种光泵预选态的原子光谱测量方法,并对Ba原子的6s5d3 D态与6p5d3 F态的超精细结构及该跃迁的同位素移动进行了直接测量。首先利用791nm的激光激发Ba原子特定同位素及特定超精细结构的6s6s 1 S0→6s6p3 P1跃迁,并利用6s6p3 P1→6s5d3 D2的自发辐射有选择地分别将这些同位素制备到6s5d3 D2态不同的超精细能级上,再用778nm的激光扫出对应的6s5d3 D2→6p5d3 F2跃迁的荧光光谱,通过这几组光谱之间的对比直接实现了对22条超精细谱线的认定和归属,从而得到了135 Ba和137 Ba的6s5d3 D2能级与6p5d3 F2能级的超精细结构常数及该跃迁的同位素移动。     

Hg绿谱线超精细结构分析及相互作用常数计算

比较了Hg的546.1 nm绿谱线超精细结构的理论计算值和实验值,定出了原子超精细结构磁偶极矩相互作用常数Am和电四极矩相互作用常数Be.     

电子性作用对MgB2超导体同位素效应的影响

通过引入电子性作用V_c,在弱耦合条件下导出了两带模型的T_c公式和同位素效应指数公式,计算了超导体MgB_2的超导转变温度和同位素效应,得到了与实验相符的结果。结果表明,带内电子性作用比带间电子性作用对同位素效应指数的影响要大。     

钕离子同位素移位和超精细结构光谱

原子光谱中,同位素移位和超精细结构光谱是少数几个能够将原子物理和原子核物理这两个不同的物理分支联系起来的课题之一.利用共线快离子束-激光光谱学方法测量了单电荷态钕离子4f45d6G3/2→(26041)°5/2跃迁(波长577.21 nm)的共振光谱,得到了所有7个稳定同位素(A=142～146,148,150)之间的能量移位和2个奇同位素(A=143,145)的超精细结构光谱.     

测定汞原子塞曼谱线相对强度

在原塞曼效应实验基础上，测定了塞曼分裂各谱线的相对强度，以作为原实验的补充．     

汞原子塞曼效应分裂谱线相对强度的测量

为了研究塞曼效应分裂谱线的相对强度,分析了Hg(546.1 nm)谱线能级在外磁场中的分裂情况,详细给出了分裂能级的量子数分布和理论相对强度;在此基础上采用CCD拍摄了分裂谱线干涉圆环的图像,并对其进行了强度分析,通过图像强度处理得到各分裂谱线相对强度与理论分析结果十分接近;表明采用CCD图像技术能较好的分析塞曼效应现象和规律.     

一价原子有精细结构时的塞曼效应

利和微扰理论导出了一价原子在静磁场中有精细结构时塞曼效应的一般表达式。     

塞曼效应实验系统评述

对塞曼效应实验系统各环节的作用、要求和关键作了分析和评述，指出了安排实验中应注意的问题，提出了观察不同谱线塞曼效应的建议．     

氖原子激发态塞曼效应的光电压光谱

本实验首次用光电压效应研究氖原子激发态的塞曼效应，并由此得到一组能级的朗德ｇ因子。     

Snake模型应用于塞曼效应分裂图谱处理

随着CCD摄像技术成熟并应用于塞曼效应实验中,图像数据的处理方法成了影响实验测量误差的最大因素.本文采用改进的可变压力Snake模型方法实现塞曼效应分裂圆环的数据测量,从而提高测量的稳定性和精确度;并利用Origin的非线性拟合进行数据的误差评价.     

气体压强对塞曼激光陀螺偏频特性的影响研究

就气体压强对激光陀螺偏频特性影响进行了理论与实验研究.理论推导发现,激光陀螺内部的He-Ne气体压强对其偏频量有重要影响.He-Ne气体比率一定时,偏频量与其内部压强成线性关系.在不同气压下对激光陀螺偏频量与压强的关系进行了实验验证,实验结果与典型参量下的理论结果吻合得较好;给出了不同比率下激光陀螺偏频量与其压强的关系曲线.     

A novel method to measure the isotope shifts and hyperfine splittings of all ytterbium isotopes for a 399-nm transition

We report the experimental results on measuring the isotope shifts and hyperfine splittings of all ytterbium isotopes for a 399-nm transition by using a quite simple and novel method.It benefits from the advantages of the modulation transfer spectroscopy in an ytterbium hollow cathode lamp and the Doppler-free spectroscopy in a collimated ytterbium atomic beam.The key technique in this experiment is simultaneously measuring the frequency separations of the two spectra twice,and the separation difference between two measurements is solely determined by the well-defined frequency of an acousto-optics modulator.Compared with the most of previously reported experimental results,ours are more accurate and completed,which will provide the useful information for developing a more accurate theoretical model to describe the interaction inside an ytterbium atom.     

Exact solution of the classical mechanical quadratic Zeeman effect

We address the curious problem of quadratic Zeeman effect at the classical mechanical level. The problem has been very well understood for decades, but an analytical solution of the equations of motion is still to be found. This state of affairs persists because the simultaneous presence of the Coulombic and quadratic terms lowers the dynamical symmetry. Energy and orbital angular momentum are still constants of motion. We find the exact solutions by introducing the concept of an image ellipse. The quadratic effect leads to a dilation of space-time, and a one-to-one correspondence is observed for pairs of physical quantities like energy and angular momentum, and the maximum and minimum distances from the Coulomb center for the Zeeman orbit and the corresponding pairs for the image ellipse. Thus, instead of finding additional conserved quantities, we find constants of motion for an additional dynamics, namely, the image problem. The trajectory is open, in agreement with Bertrand’s theorem, but necessarily bound. A stable unbound trajectory does not exist for real values of energy and angular momentum. The radial distance, the angle covered in the plane of the orbit, and the time are uniquely determined by introducing further the concept of an image circle. While the radial distance is defined in a closed form as a transcendental function of the image-circular angle, the corresponding orbit angle and time variables are found in the form of two convergent series expansions. The latter two variables are especially contracted, thereby leading to a precession of the open cycles around the Coulomb center. It is expected that the space-time dilation effect observed here would somehow influence the solution of the quantum mechanical problem at the non-relativistic level.