Because the final
state of the scattering system has greater energy than the initial
state, the observed spectral features are, strictly, Stokes
lines (e.g., Bransden & Joachain 1983). We will refer to them as
Raman lines, both because this has become the established terminology in
astronomical applications, and to avoid possible confusion which may
result from the separate requirement of discussing the Stokes
parameters.
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