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6 - The excitation of fine structure transitions

Published online by Cambridge University Press:  12 October 2009

David Flower
Affiliation:
University of Durham
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Summary

Introduction

An important cooling process in interstellar clouds is the excitation of fine structure transitions in abundant atoms and ions, followed by radiative decay. The relevant transitions are those between the fine structure components of ground terms, such as C0 2p2 3P, O0 2p4 3P and C+ 2p 2Po. By term is meant the LS-coupling state denoted by 2S+1L, where L is the total electronic orbital angular momentum quantum number and S is the total electronic spin angular momentum quantum number. Only the outer (valence) electrons (e.g. 2p2) need to be listed, as the inner shells and sub-shells are closed and have zero resultant angular momenta. Spectrosopic notation is used to denote the orbital angular momentum: ‘s’ for l = 0, ‘p’ for l = 1, ‘d’ for l = 2, …, with upper case letters indicating resultant angular momenta (vector sums of the contributions of the individual valence electrons). Departures from LS-coupling, owing to the spin—orbit interaction, result in the states with different values of J, the total electronic angular momentum (the vector sum of the orbital and spin angular momenta) having slightly different energies; these fine structure states are denoted 2S+1LJ. Thus the ground 3P term of C0 and O0 is a triplet, comprising the three fine structure components with J = 0, 1, 2, and the 2Po ground term of C+ is a doublet with J = 1/2, 3/2.

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Publisher: Cambridge University Press
Print publication year: 2007

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