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锂原子

锂原子的相关文献在1981年到2022年内共计72篇,主要集中在物理学、化学、电工技术 等领域,其中期刊论文63篇、会议论文7篇、专利文献54249篇;相关期刊36种,包括安徽大学学报(自然科学版)、安徽师范大学学报(自然科学版)、现代材料动态等; 相关会议6种,包括第八届全国大学生创新创业年会、中国核学会2015年学术年会、2013年中国工程热物理学会传热传质学学术年会等;锂原子的相关文献由124位作者贡献,包括柴俊杰、王治文、钱兴中等。

锂原子—发文量

期刊论文>

论文:63 占比:0.12%

会议论文>

论文:7 占比:0.01%

专利文献>

论文:54249 占比:99.87%

总计:54319篇

锂原子—发文趋势图

锂原子

-研究学者

  • 柴俊杰
  • 王治文
  • 钱兴中
  • 何兴虹
  • 王沂轩
  • 王鹏
  • 黄时中
  • CHAI Jun-jie
  • 余世英
  • 冯泽
  • 期刊论文
  • 会议论文
  • 专利文献

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    • 张志才; 马良财
    • 摘要: 本文基于第一性原理计算,系统地研究了碱金属Li原子修饰缺陷蓝磷单层体系的储氢性能.研究结果表明,双空位缺陷DV2的引入可以有效增强Li原子与蓝磷单层间的相互作用,能够有效阻止单层表面Li团簇的形成.单个Li原子可以稳定吸附3个H_(2)分子,H_(2)分子平均吸附能为0.248eV/H_(2).电子结构分析表明,H_(2)分子主要通过极化机制和轨道杂化作用吸附在Li修饰的缺陷蓝磷单层体系上.此外,本文还研究了温度和压强对Li/DV2体系储氢性能的影响.结果表明,在室温和低压条件下,H_(2)分子可以稳定吸附在Li/DV2体系表面,从而实现室温条件下的可逆储氢.
    • 张启迪; 李鹏程; 赵松峰; 周效信
    • 摘要: 利用单电子近似下锂原子精确的模型势,通过数值求解三维含时薛定谔方程的方法,研究了锂原子在激光场中发射低阶谐波的性质,研究结果表明,对于锂原子电离阈值以下的低阶谐波,除了通常的奇次谐波外,还有侧峰结构出现,运用同步压缩变换技术(SST)分析这些低阶谐波的辐射特性,我们发现这些侧峰是由原子在激光场中的缀饰态之间的跃迁和无场下激发态到基态的跃迁组成的,如果当激光脉冲结束后,仍有发射的侧峰,其位置与主峰之间的能量差可以用来估算原子激发态在激光场中的最大Stark移动.
    • 董良杰
    • 摘要: 在量子力学中,我们常用变分法和微扰法来求解近似问题.但在运用微扰法计算过程中,微扰项必须很小才可以使用,很难求精确解,对解决某些特定问题具有一定的局限性.而变分法则不受此限制.为此,下面运用变分法通过计算对基态锂原子的能量和波函数进行探解.
    • 戚晓秋; 刘冬丽; 戴长建
    • 摘要: The quantum statistical weight (G) of an atomic energy level is an important spectroscopic parameter,its effect on the atomic ionization process is,however,usually neglected for simplicity.In this work,the influences of the G parameters of the lithium atomic energy levels are taken into account explicitly for the first time in the study on the process of three-step photo-excitation (PE) + electric field ionization (EFI),which yields a significant effect on overall EFI efficiency of the PE+EFI process.With a set of specially designed PE+EFI schemes,the expected results are obtained.First,with a three-step PE scheme,the Li atom is excited by three pulsed lasers with different wavelengths,which are fired simultaneously,to one of the Rydberg states from its ground state,from which the Li atom is ionized by an electric-field pulse with a time delay in order to avoid the Stark effect.Based on the three physical processes the atom experiences the PE,none field,and the EFI processes,and a set of universal rate equations are established according to the conservation law of particle number with the knowledge of physical mechanism of the three different processes and the physical model set up for them,respectively.The G parameters of the four relevant bound energy states are displayed explicitly in the rate equations for the PE process to offer a clear viewabout their effect on the overall EFI efficiency of the PE+EFI process.Secondly,the overall efficiencies of PE+EFI process are calculated with the Matlab programming for the two specified excitation schemes,2S1/2--→ 2P1/2 → 3S1/2 → 25P1/2,3/2 and 2S1/2 → 2P3/2 → 3D5/2 → 25F5/2,7/2.The overall EFI efficiency of PE+EFI process is investigated not only by adjusting the laser parameters but also by comparing the results between the two different excitation schemes.In order to establish the relationship between the overall EFI efficiency and external field quantitatively,the dependence of population rate of the relevant bound states on various factors,such as laser and atomic parameters,is calculated systematically.The role of the G parameters of the relevant atomic energy levels played in the population rates is observed to determine which excitation scheme is better in terms of the population rate of the Rydberg state.Meanwhile,the spontaneous emission of the Rydberg state during the time delay between the pulses of electric field and laser is also evaluated to make a balance between avoiding the Stark effect and minimizing the spontaneous emission.Based on the analysis of the calculations,some new results are achieved.An enhancement of the overall EFI efficiency can be obtained by making a sophisticated design on the excitation scheme of the PE+EFI process to optimize the G parameters.The time delay between the pulses of electric field and laser not only lets the atom experience a field-free time period,but also makes an upper limit for the population rate of Rydberg state due to the redistribution of atom among the four relevant bound states in the period.The upper limit is found to be dependent on neither laser parameters nor the absolute values of the G parameters,while only on the branching ratio of the G parameters among those bound states.The overall EFI efficiency is dominated by the population rate of Rydberg state,as the EFI process may ionize all Rydberg atoms once the strength of the EFI field reaches the EFI threshold of the Rydberg state.Hence,the key factor for raising the overall EFI efficiency is to enhance the population rate of Rydberg state in the PE process,which is a hard challenge due to the upper limit for the population rate of Rydberg state.%原子能级的量子统计权重(G)是原子的重要光谱参数,但在研究原子的电离过程中通常却为了简化问题而被忽略.本文在锂原子的三步光激发(PE)+电场电离(EFI)过程中计入了其影响,并发现其对原子EFI效率的影响显著.本文精心设计了一套锂原子的PE+EFI方案:首先,采用三台不同波长的脉冲激光器分三步将原子从基态激发到某一Rydberg态上,经过一段时间延迟后再施加脉冲电场将其电离.针对原子所经历的PE、零场和EFI这三个物理过程,本文对其物理机制进行了分析并建立了服从粒子数守恒的物理模型进而导出了显含G参数的普适的速率方程组.其次,通过Matlab编程,分别针对精心选定的两条激发路径2S1/2→2P1/2→3S1/2→25P1/2,3/2和2S1/2→2P3/2→3D5/2→25F5/2,7/2开展了数值计算.研究发现:PE+EFI过程的总体效率的上限既与激光参数无关,也不依赖于G参数的绝对值,而是决定于Rydberg态的G参数的分支比.总之,通过精选激发路径可以调控PE过程各相关态的布居率,并能适当提高PE+EFI过程的总电离效率,但却因受到Rydberg态布居率的限制而很难进一步提高.
    • 摘要: 加拿大不列颠哥伦比亚大学(UBC)的物理学家称他们通过在石墨烯上面涂覆锂原子,首次制备出了超导石墨烯样品。虽然之前在夹层块状石墨中已经观察到了超导性,但直到现在科学家还未发现超导单层石墨烯。
    • 瞿定荣; 范凤英; 宋增云
    • 摘要: In this paper, collisional quenching rate for Li(2P ) atoms with argon molecules is studied in photochemical isotope separations. In the weak laser irradiation, the absorption spectra and fluorescence emission spectra of lithium atom vapor is measured by changing the argon pressure. The quenching rate constant of (12.29 ± 0.92) × 10-18 m3·s-1 for Li(2P ) atoms quenched with argon molecules have been determined. This value is much smaller than the spontaneous emission rate of Li(2P ) atoms. The experimental result shows that in photochemical lithium isotope separation collisional quenching effect on the separation selectivity is very small and can be neglected.%本文对光化学法分离中氩气对2P激发态锂原子的碰撞猝灭速率进行研究.在弱激光作用下,通过对不同氩气压强下的锂原子蒸气吸收光谱和激发态锂原子的荧光发射光谱进行测量,得到氩气对2P激发态锂原子的猝灭速率常数为(12.29±0.92)×10-18 m3·s-1.实验结果表明:在光化学锂同位素分离研究中,氩气对锂原子2P激发态的猝灭速率远小于2P激发态锂原子的自发辐射速率,碰撞猝灭效应对分离选择性的影响非常小,可以忽略不计.
    • 董丽(摘译)
    • 摘要: 休斯顿密歇根理工大学的副教授Reza Shahbaziano-Yassar开发出一种新装置,使研究人员能监测单个锂原子并有可能开发出下一代锂电池。
    • 李增; 黄时中
    • 摘要: 以最弱受约束电子模型理论(WBEPM)所得到的锂原子基态波函数为基础,利用Gao和Starace提出的稳定变分方法,计算了锂原子的电多极极化率和锂-锂体系的两体色散系数,计算结果与已有文献吻合,但计算方法更为简化且便于推广到其他碱金属原子.
    • 方敏; 王君
    • 摘要: 采用处理慢电子被原子散射的等效势模型,计算能量在0.1~15 eV范围内电子与锂原子系统的弹性散射总截面和微分截面,并把计算结果与一些实验和理论值进行对比,结果吻合较好.另讨论了Hammerling交换势中比例系数γ取不同数值时对结果的影响.
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