...
首页> 外文期刊>The European physical journal, D. Atomic, molecular, and optical physics >Stark broadening of isolated lines: calculation of the diagonal multiplet factor for complex configurations (n(1)l(1)(n) n(2)l(2)(m) n(3)l(3)(p))
【24h】

Stark broadening of isolated lines: calculation of the diagonal multiplet factor for complex configurations (n(1)l(1)(n) n(2)l(2)(m) n(3)l(3)(p))

机译:隔离线的明显加宽:复杂配置(n(1)l(1)(n)n(2)l(2)(m)n(3)l(3)(p)的对角线多重因子的计算

获取原文
获取原文并翻译 | 示例
   

获取外文期刊封面封底 >>

       

摘要

Owing to the increasing sensitivity of detectors, accurate line profiles are needed for accurate stellar atmospheres modelling and for laboratory and technological plasmas as well. So, Stark broadening parameters of isolated lines of complex atoms and ions within the impact and quasistatic approximation are needed, even if the atomic abundance of the considered element is low. Angular factors of the diagonal line strength entering the quadrupole term appearing in the semi-classical expression of the width of line broadened by electron or ion perturbers, are needed. The aim of this paper is to extend the previous calculations of this diagonal multiplet factor which were obtained for configurations of the type l(n) and l(1)(n)l(2)(m) to more complex configurations in LS coupling. To study the Stark broadening of isolated lines in the impact and quasistatic approximation, we use the semi-classical-perturbation treatment, including both dipole and quadrupole contribution in the expansion of the electrostatic interaction between the optical electron and the perturber. We also use the Fano-Racah algebra. Angular factors of the diagonal line strength entering the quadrupole term appearing in the semi-classical expression of the width of line broadened by electron or ion perturbers, are calculated. New diagonal multiplet factor formulae for more complicated configurations such as (n(1)l(1)(n)(LnSn) n(2)l(2)(m)(LmSm) n(3)l(3)(p)(LpSp)) are provided. These formulae can enter the computer Stark semi-classical perturbation codes.
机译:由于探测器灵敏度的提高,需要精确的线轮廓来进行准确的恒星大气建模以及实验室和技术等离子体。因此,即使所考虑元素的原子丰度较低,也需要在撞击和准静态逼近内形成复杂原子和离子的隔离线的Stark加宽参数。需要进入四极项的对角线强度的角因子出现在被电子或离子扰动加宽的线宽的半经典表达式中。本文的目的是将对角线多重因子的先前计算扩展到LS耦合中的更复杂的配置,该计算是针对类型为l(n)和l(1)(n)l(2)(m)的配置而获得的。 。为了研究碰撞和准静态逼近中孤立线的Stark拓宽,我们使用半经典扰动处理,包括偶极子和四极子对光学电子和扰动子之间静电相互作用扩展的贡献。我们还使用Fano-Racah代数。计算通过电子或离子扰动加宽的线宽的半经典表达式中出现的进入四极项的对角线强度的角因子。用于更复杂配置的新对角线多重因子公式,例如(n(1)l(1)(n)(LnSn)n(2)l(2)(m)(LmSm)n(3)l(3)(p )(LpSp))。这些公式可以输入计算机Stark半经典扰动代码。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号