双掺(Tm3+,Tb3+)LiYF4激光器1.5 μm波长激光阈值分析

由速率方程推出了双掺（Tm^3 ,Tb^3 ）离子准四能级系统的激光阈值解析式，讨论了Tm^3 和Tb^3 离子之间的相互作用。分析了1.5μm波长附近的激光阈值和Tm^3 、Tb^3 离子的掺杂原子数分数及晶体长度的关系。结果表明，对于对应Tm^3 离子^3H4→^3F4跃迁的约1.5μm波长的激光，激活离子Tm^3 的掺杂原子数分数过大时，交叉弛豫作用将使系统阈值迅速增加。Tb^3 离子的加入，一方面能抽空激光下能级，起到降低阈值的作用；另一方面亦减少了激光上能级的寿命，使阈值升高。故Tb^3 离子有最佳掺杂原子数分数。对于Tm原子数分数为y=0.01的Tm:LiYF4晶体，Tb^3 离子的最佳掺杂原子数分数为0.002左右，同时表明，激光阈值与晶体长度有关。最佳晶体长度与Tm^3 、Tb^3 离子的掺杂原子数分数以及晶体的衍射损耗和吸收损耗有关。     

物理学咬文嚼字之三十六 Στοιχειαιο

Euclid的《几何原本》同化学术语中的化学计量比都来自希腊语Στοιχεια■ο,反映的是古希腊原子论的精神.     

费米气体在调制缺陷晶格中的超流特性

本文研究了费米气体在调制缺陷的一维环形光晶格中的超流特性．在流体动力学模型和两模近似下,整个系统的动力学性质可以等效为单摆模型的哈密顿量,从而得到系统发生超流相变的临界条件ρc ．系统在BEC-BCS整个渡越区中,临界原子数密度将使得系统存在缺陷导致阻尼的正常态之外的另一种状态,即平面波连续穿过缺陷的超流态．系统的超流特性依赖于缺陷的强度、类型以及原子间的相互作用,并且由于缺陷与原子间相互作用的耦合,系统在BCS端更容易维持超流态。     

Atomic Tunneling Effect in Two-Component Bose-Einstein Condensates with a Coupling Drive

In this paper, we have studied the atomic population difference and the atomic tunneling current of two-component Bose-Einstein condensates with a coupling drive. It is found that when the two-component Bose Einstein condensates are initially in the coherent states, the atomic population difference may exhibit the step structure, in which the numbers of the step increase with the decrease of the Rabi frequency and with the increment of the initial phase difference. The atomic population difference may exhibit collapses, and revivals, in which their periods are affected dramatically by the Rabi frequency and the initial phase difference. The atomic tunneling current may exhibit damping oscillation behaviors, and exist the step structure for the time range of 10^-10 ～ 10^-9 second.     

DFT Study on a Heterofullerene C_(58)Sn with Odd Number of Atoms

Density functional theory calculations and structural minimization techniques have been employed to characterize the structural and electronic properties of [5,6]-heterofullerene-C58Sn-C2. Since the heterofullerene molecule CssSn has a nearly planar tetra-coordinated Sn atom on the skeleton of cage, it is a heterofullerene molecule with odd number of atoms and a novel molecule. Vibrational frequencies of the molecule have been calculated at the B3LYP/CEP-31G level of theory. The absence of imaginary vibrational frequency confirms that the molecule corresponds to a true minimum on the potential energy hypersurface, and its heat of formation was estimated in this study. Owing to the C2 symmetry of [5,6]-heterofullerene-C58Sn-C2, it is a chiral molecule.     

Determination of the number of atoms of the long-lived nuclide 126Sn by γ-ray spectrometry

By using HPGe γ-ray spectrometry, the activity of the long-lived fission product 126Sn in a SnOB2 sample was measured. The number of 126Sn atoms and the ratio of 126Sn to Sn were calculated based on the half-life value of 2.35×105a and the chemical stoichiometry. The result of the ratio of 126Sn to Sn, （1.033±0.037）×10-8, is consistent with the results measured by the accelerator mass spectrometry （AMS） within uncertainty limits, which confirms our procedures in the measurement of 126Sn by AMS and lays a foundation for the AMS measurement of 126Sn at much lower levels.     

Effects of atomic number Z on the energy distribution of hot electrons generated by femtosecond laser interaction with metallic targets

The effects of atomic number Z on the energy distribution of hot electrons generated by the interaction of 60fs, 130mJ, 800nm, and 7×10^17W/cm^2 laser pulses with metallic targets have been studied experimentally. The results show that the number and the effective temperature of hot electrons increase with the atomic number Z of metallic targets, and the temperature of hot electrons are in the range of 190-230keV, which is consistent with a scaling law of hot electrons temperature.     

光晶格钟为守时设立新标准

<正>这类钟的优势在于使用的原子数量;它不是按照单个原子的节奏嘀嗒走针,而是同时与几千个原子同步。从1955年原子钟出现至今,量子时间计量的准则一直没有改变:将原子与外场隔离,调谐相干辐射源频率到原子跃迁,并通过对辐射振荡周期的计数来测量时间。     

紫外光诱导原子脱附技术在单腔磁阱装载中的应用

基于光诱导的原子脱附技术，采用脉冲紫外光剥离出玻璃池壁上吸附的铷原子以形成可快速开启和关断的脉冲铷原子源，成功地解决了单真空腔系统中磁阱的原子数和寿命之间的矛盾，突破了激光冷却和囚禁技术向小型化乃至微型化发展过程中的一个瓶颈.脉冲光源由390nm的LED阵列组成.实验结果表明它能够在1s内使真空铷原子气体分压提高近30倍,并且当紫外光关闭后系统的真空恢复到平衡状态的时间非常短，约120ms.测量了不同铷原子分压下磁光阱所俘获的最大原子数和装载时间,并由此得出系统的背景真空和磁光阱所能俘获的极限原子数，进一步得出磁阱的原子数-寿命积与磁光阱保持阶段时间的变化关系，结果显示在约1.25s处出现极大值，与无磁光阱保持阶段而直接进行磁阱装载情况相比提高了约0.3倍. 关键词： 激光冷却 磁光阱 光诱导原子脱附 原子数-寿命积