4.5 Article

Transition properties of X1 Σ+, A1Σ-, B1 Δ, C1 Π, a3 Σ+, b3 Δ, c3 Π, and d3 Σ- states of PO+

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jqsrt.2021.107553

Keywords

PO+ cation; Radiative lifetimes; Symmetry-forbidden transitions; Einstein A coefficients; Spin-forbidden transitions

Funding

  1. National Natural Science Foundation of China [12074105]

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This study calculated the potential energy curves and transition dipole moments between different states of PO+ using various methods, taking into account core-valence correlation, scalar relativistic corrections, and spin-orbit coupling. The results showed variations in the radiative lifetimes and intensities of different transitions, providing useful guidelines for detection in future experiments.
The potential energy curves of the X-1 Sigma(+), A(1) Sigma(-), B-1 Delta, C-1 Pi, a(3) Sigma(+), b(3) Delta, c(3) Pi, and d(3) Sigma(-) states of PO+ and the transition dipole moments between these states were calculated using the CASSCF method, and then the icMRCI approach. To accurately compute the transition properties, core-valence correlation and scalar relativistic corrections were taken into account. The spin-orbit coupling calculations were used to determine the transition properties of the A(1) Sigma(-), B-1 Delta, a(3) Sigma(+), and b(3) Delta states, from which no spontaneous emissions were generated owing to the limitations from the dipole-allowed transition selection rule. The radiative lifetime was approximately 10 - 100 ns for the C-1 Pi state and 10 mu s for the c(3) Pi state. Among these dipole-allowed transitions, the emissions from the C-1 Pi - X-1 Sigma(+) system was the strongest and was followed by the C-1 Pi - A(1)Sigma(-) and c(3) Pi - a(3) Sigma(+) transitions. The radiative lifetime was approximately 10 - 100, 10 - 100, and 100 mu s for the A(1) Sigma(-)(0), d(3) Sigma(-)(0+), and d(3) Sigma(-)(1) states, respectively. Those were of the order of 0.1 - 10, 10, 10 - 100, 1 - 100, and 0.1 - 1 ms for the B-1 Delta(2), a(3) Sigma+(1), a(3) Sigma(+)(0-), b(3)Delta(1), and b(3)Delta(2) states, respectively. Among the spontaneous emissions generated from these Omega states, those from the A(1)Sigma(-)(1) - a(3)Sigma+(0-), A(1)Sigma(-)(1) - a(3)Sigma(+)(1), B-1 Delta(2) - b(3)Delta(3), b(3)Delta(2) - a(3)Sigma+(1), d(3)Sigma(-)(0+) - a(3)Sigma(+)(0-), and d(3)Sigma(-)(1) - a(3)Sigma+(1) transitions were relatively strong. The transition properties reported herein are expected to provide useful guidelines for the detection in future experiments. (C) 2021 Elsevier Ltd. All rights reserved.

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