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以多电子原子精细结构哈密顿的球张量形式和氦原子非相对论性能级结构理论为基础,借助不可约张量理论,建立了计算氦原子自旋-其它轨道相互作用精细结构参数的一种解析理论形式.完成了所有的角向积分和自旋求和计算,自旋-其它轨道相互作用精细结构参数最终用若干个径向积分来表示.以氦原子(1s2p)3P态为例,借用类氢形式的径向函数对这些径向积分进行了近似计算.计算结果表明:在氦原子的精细结构中,自旋-其它轨道相互作用与纯自旋-轨道相互作用的作用效果相反;在总自旋-轨道相互作用精细结构参数中,自旋-其它轨道相互作用起决定性作用,它决定着精细结构分裂的顺序. 相似文献
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本文借助不可约张量理论,导出了通常由光谱实验数据确定的氦原子sp组态自旋-轨道相互作用精细结构参数A的理论计算式,在推导过程中完成所有角向积分和自旋求和计算. 相似文献
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类Na离子里德堡态的势模型波函数和极化率 总被引:1,自引:1,他引:0
本文采用一种改进的原子唯象模型,获得了类钠离子高里德堡态(8≤n≤30)解析形式的价电子波函数。由此系统地计算了MgⅡ、AlⅢ、SiⅣ、PⅤ、SⅣ、ClⅦ、ArⅧ、KⅨ离子相应里德堡态的标量和张量极化率,并建立了极化率与主量子数的标度关系。文中还对极化率随离化度的变化规律进行了讨论。 相似文献
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绿宝石晶体自旋二重态对基态能级的影响及Jahn-Teller效应 总被引:5,自引:2,他引:5
应用不可约张量方法和群的理论构造了三角对称晶场中考虑自旋 轨道相互作用,自旋 自旋相互作用和自旋 其它轨道相互作用的3d3/3d7态离子的可完全对角化的120阶微扰哈密顿矩阵.利用该矩阵计算了绿宝石晶体的基态能级、零场分裂参量,研究了自旋二重态对基态能级的贡献.理论计算值与实验值相符合,证明二重态对基态的贡献是不可忽略的.在此基础上,进一步研究了自旋 自旋相互作用、自旋 其它轨道相互作用和自旋 轨道相互作用对绿宝石晶体的光谱精细结构和零场分裂参量的影响,发现自旋 自旋和自旋 其它轨道相互作用对绿宝石晶体基态能级和零场分裂参量的影响都是不可忽略的.从而通过理论计算值和实验值的比较,证实了在绿宝石晶体中Jahn Teller效应的存在,它能够对光谱精细结构的分裂提出一些更加合理的解释. 相似文献
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计算了Na原子d电子系列Rydberg态的精细结构,获得与实验值相一致的结果。精细结构倒置的原因主要是介电子和原子实的交换作用,并发现原子实玫极化作用与有较大的贡献。计算过程中,在准相对论的框架下,用自旋极化模型,考虑了原子实与价电子的相互作用,采用自洽场方法,计算了原子实和价电子物径向波函数以及能量。原子;实采用自相互作用修正的Xα(SIC-Xα)方法,价电子波函数考虑到了价电子的自旋-轨道耦合作 相似文献
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利用双中心原子轨道强耦合方法研究了H^+离子与里德堡态的Li(5d)原子碰撞的电荷转移过程,计算了5d电子转移到氢原子各个次壳层的态选择截面及总截面.研究了态选择截面随俘获电子主量子数及角量子数变化的规律,并尝试给出了解析的标度关系;探讨了标度规律随入射粒子能量的变化,分析了高激发态电子电荷转移过程的动力学机制. 相似文献
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J. E. Palmer 《Molecular physics》2019,117(21):3108-3119
Matter-wave interferometry has been performed with helium atoms in high Rydberg states. In the experiments the atoms were prepared in coherent superpositions of Rydberg states with different electric dipole moments. Upon the application of an inhomogeneous electric field, the different forces on these internal state components resulted in the generation of coherent superpositions of momentum states. Using a sequence of microwave and electric field gradient pulses the internal Rydberg states were entangled with the momentum states associated with the external motion of these matter waves. Under these conditions matter-wave interference was observed by monitoring the populations of the Rydberg states as the magnitudes and durations of the pulsed electric field gradients were adjusted. The results of the experiments have been compared to, and are in excellent quantitative agreement with, matter-wave interference patterns calculated for the corresponding pulse sequences. For the Rydberg states used, the spatial extent of the Rydberg electron wavefunction was ~320?nm. Matter-wave interferometry with such giant atoms is of interest in the exploration of the boundary between quantum and classical mechanics. The results presented also open new possibilities for measurements of the acceleration of Rydberg positronium or antihydrogen atoms in the Earth's gravitational field. 相似文献
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Studying the complex quantum dynamics of interacting many-body systems is one of the most challenging areas in modern physics. Here, we use machine learning (ML) models to identify the symmetrized base states of interacting Rydberg atoms of various atom numbers (up to six) and geometric configurations. To obtain the data set for training the ML classifiers, we generate Rydberg excitation probability profiles that simulate experimental data by utilizing Lindblad equations that incorporate laser intensities and phase noise. Then, we classify the data sets using support vector machines (SVMs) and random forest classifiers (RFCs). With these ML models, we achieve high accuracy of up to 100% for data sets containing only a few hundred samples, especially for the closed atom configurations such as the pentagonal (five atoms) and hexagonal (six atoms) systems. The results demonstrate that computationally cost-effective ML models can be used in the identification of Rydberg atom configurations. 相似文献
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A computational procedure for controlling the stochastic ionization of one-dimensional single electron Rydberg atoms in the correspondence principle regime is developed. Using our procedure it is possible to suppress excitation and ionization of the one-dimensional Rydberg atom even in strong microwave fields for which ionization would otherwise be instantaneous. 相似文献
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M. R. Flannery E. Oks 《The European Physical Journal D - Atomic, Molecular, Optical and Plasma Physics》2008,47(1):27-31
A Rydberg atom embedded in a plasma can experience penetration by slowly moving electrons within its volume. The original
pure Coulomb potential must now be replaced by a screened Coulomb potential which contains either a screening length Rs or a screening factor A = Rs
-1 . For any given discrete energy level, there is a Critical Screening Factor (CSF) Ac beyond which the energy level disappears (by merging into the continuum). Analytical results are obtained for the classical
dependence of the energy on the screening factor, for the CSF, and for the critical radius of the electron orbit for Circular
Rydberg States (CRS) in this screened Rydberg atom. The results are derived for any general form of the screened Coulomb potential
and are applied to the particular case of the Debye potential. We also show that CRS can temporarily exist above the ionization
threshold and are therefore the classical counterparts of quantal discrete states embedded into continuum. The results are
significant not only to Rydberg plasmas, but also to fusion plasmas, where Rydberg states of multi-charged hydrogen-like ions
result from charge exchange with hydrogen or deuterium atoms, as well as to dusty/complex plasmas. 相似文献
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Yafen Cai Shuai Shi Yijia Zhou Jianhao Yu Yali Tian Yitong Li Kuan Zhang Chenhao Du Weibin Li Lin Li 《Frontiers of Physics》2023,18(1):12302
Stabilizing important physical quantities to atom-based standards lies at the heart of modern atomic, molecular and optical physics, and is widely applied to the field of precision metrology. Of particular importance is the atom-based microwave field amplitude stabilizer, the so-called atomic candle. Previous atomic candles are realized with atoms in their ground state, and hence suffer from the lack of frequency band tunability and small stabilization bandwidth, severely limiting their development and potential applications. To tackle these limitations, we employ microwave-dressed Rydberg atoms to realize a novel atomic candle that features multi-band frequency tunability and large stabilization bandwidth. We demonstrate amplitude stabilization of microwave field from C-band to Ka-band, which could be extended to quasi-DC and terahertz fields by exploring abundant Rydberg levels. Our atomic candle achieves stabilization bandwidth of 100 Hz, outperforming previous ones by more than two orders of magnitude. Our simulation indicates the stabilization bandwidth can be further increased up to 100 kHz. Our work paves a route to develop novel electric field control and applications with a noise-resilient, miniaturized, sensitive and broadband atomic candle. 相似文献
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本文主要研究了调制探测激光场中铯Rydberg 原子阶梯型三能级系统的电磁感应透明(EIT) 效应. 铯原子基态6S1/2, 第一激发态6P3/2 和Rydberg 态形成阶梯型三能级系统, 探测光作用于6S1/2 (F = 4)→6P3/2(F' = 5) 的跃迁, 耦合光在Rydberg 跃迁线6P3/2→49S1/2 附近扫描, 形成Rydberg 原子EIT. 当对探测光频率施加一个几kHz 的调制时, 调制解调后的EIT 信号分裂为两个峰, 双峰间距与调制频率无关,而与调制幅度导致的失谐量大小(频率调制幅度) 成正比, 双峰间隔的一半等于探测光频率调制幅度的λp/λc = 1.67 倍. 实验结果与理论计算相一致. 本文的研究结果可应用于激光线型和频率抖动的实时监测. 相似文献
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The radiative lifetimes of the Eu 4f76snp(8PJ or10PJ)Rydberg states with J=5/2 and 11/2 are investigated with a combination of multi-step laser excitation and pulsed electric field ionization,from which their dependence on the effective principal quantum number is observed.The lifetimes of 21 states are reported along with an evaluation of their experimental uncertainty.The influence of blackbody radiation,due to the oven temperature,on the lifetime of the higher-n states is detected.The non-hydrogen behavior of the investigated states is also observed. 相似文献
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