Branching ratios of radiative transitions in O VI

TL;DR

This study calculates the branching ratios of radiative transitions in O VI using relativistic coupled cluster theory, revealing patterns and trends among electric and magnetic transition probabilities with good agreement to existing data.

Contribution

First application of relativistic coupled cluster theory to compute radiative transition branching ratios in O VI, providing detailed analysis and validation against known data.

Findings

Electric quadrupole ($E2$) transitions generally have higher probabilities than magnetic dipole ($M1$) transitions.

Transition probabilities vary depending on the involved levels and their fine structure.

Calculated lifetimes of excited states match well with existing experimental and theoretical results.

Abstract

We study the branching ratios of the allowed and forbidden radiative transitions among the first few (9) fine structure levels of O VI using relativistic coupled cluster theory. We find irregular patterns for a number of transitions with in $n$-complexes with $n\le4$. We have used the exisiting values of the allowed electric dipole ($E1$) transition as a benchmark of our theory. Good agreement with the existing values establish accuracies of not only the theoretical method but the basis function as well. In general the electric quadrupole ($E2$) transition probabilities are greater in magnitude than magnetic dipole ($M1$) transition probabilities, whereas for medium atomic transition frequencies they are of the same order of magnitude. On the other hand if the transitions involved are between two fine structure components of the same term, then the $M1$ transition probability is more probable than that of $E2$. We have analyzed these trends with physical arguments and order of magnitude estimations. The results presented here in tabular and graphical forms are compared with the available theoretical and observed data. Graphical analysis helps to understand the trends of electric and magnetic transitions for the decay channels presented here. Our calculated values of the lifetimes of the excited states are in very good agreement with the available results.