Collisional quenching of the pionic helium 4He long-lived states

A. V. Bibikov, G. Ya. Korenman, S. N. Yudin
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Abstract

Collisions of metastable pionic helium atoms with helium atoms of the medium lead to the destruction of these states, as well as to the shifts and broadening of E1 spectral lines of transitions between the pionic helium states. In the paper, in order to obtain the interaction potential matrix (π −He+)−He, calculations of the potential energy surface (PES) in the unrestricted Hartree-Fock method are performed taking into account electron correlations within the second-order perturbation theory (MP2). With this potential, the system of equations of strong channel coupling is solved numerically. Various techniques are used in the calculations that eliminate degeneracy of the solution matrix in the vicinity of small distances between colliding subsystems, which arises due to strong coupling of channels in this region, owing to which the numerical solutions “forget” boundary conditions. Cross sections and rates of collisional transitions are calculated (Nσv). It is found that the collisional transition rate (n, l) = (17, 16) → (17, 15) (n, l — the principal quantum number and the angular momentum respectively) for the density of the medium N = 0.2 × 1023 cm−3 is lower than 103s−1, which indicates that it is possible to ignore the effect of collisional destruction of pionic helium long-lived states in precision laser spectroscopic experiments.
电子氦4He长寿命态的碰撞猝灭
亚稳离子氦原子与介质中氦原子的碰撞导致了这些态的破坏,也导致了介子氦态之间跃迁的E1谱线的位移和展宽。为了得到相互作用势矩阵(π−He+)−He,本文在二阶微扰理论(MP2)中考虑电子相关,用不受限制的Hartree-Fock方法计算了势能面(PES)。利用该势,对强通道耦合方程组进行了数值求解。在计算中使用了各种技术来消除在碰撞子系统之间的小距离附近的解矩阵的退化,这种退化是由于该区域通道的强耦合引起的,因此数值解“忘记”了边界条件。计算了碰撞跃迁的截面和速率(Nσv)。发现密度为n = 0.2 × 1023 cm−3的介质的碰撞跃迁速率(n, l) =(17,16)→(17,15)(n, l分别为主量子数和角动量)小于103s−1,表明在精密激光光谱实验中可以忽略离子氦长寿命态碰撞破坏的影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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