C. Jonin et al., High-resolution electron-impact emission of H-2. I. Cross sections and emission yields 900-1200 angstrom, ASTROPH J S, 129(1), 2000, pp. 247-266
High-resolution (Delta lambda = 115 m Angstrom) emission spectra of molecul
ar hydrogen produced by electron-impact excitation at 100 eV have been obta
ined in the wavelength range 900-1200 A. The emission spectra can be assign
ed to transitions between the X (1)Sigma (+)(g) ground state and the 1s sig
ma (g)np sigma (1)(u)Sigma (u), and 1s sigma (g)np pi, (1)Pi (u) Rydberg st
ates. Synthetic rotational line spectra based on the excitation function of
Liu et al. and calculated 2p sigma B (1)Sigma (+)(u)-X (1)Sigma (+)(g), 2p
pi C (1)Pi (u)-X 1 Sigma (+)(g), 3p sigma B' (1)Sigma (+)(u)-X (1)Sigma ()(g) and 3p piD (1)Pi (u)-X (1)Sigma (+)(g) transition probabilities of Abg
rall et al. are generally found to be in good agreement with the experiment
al spectra in the regions where emissions from 1s sigma (g) np sigma (u) (n
greater than or equal to 4) and 1s sigma (g) np pi (u) (n greater than or
equal to 4) states are negligible. Emission cross sections for D (1)Pi (+)(
u), D' (1)Pi (u), and D " (1)Pi (-)(u), B' 1 Sigma (+)(u), and B " (1)Sigma
(+)(u) states are obtained by measuring the emission intensities from thes
e states relative to those from the B (1)Sigma (+)(u),C (1)Pi (u), and D (1
)Pi (-)(u) states. A high- resolution EW calibration technique is establish
ed. At 100 eV the emission cross sections of the D (1)Pi (u), D' 1 Pi (u),
D " (1)Pi (u), B' 1 Sigma (+)(u), and B " (1)Sigma (+)(u) states are measur
ed to be (2.8+/-0.4) x 10(-18), (6.3 +/- 1.3) x 10(-19), (5.9 +/- 1.7) x 10
(-20), (2.1 +/- 0.3) x 10(-18), and (1.6 +/- 0.4) x 10(-19) cm(2), respecti
vely. In addition, the vibrational emission cross sections have been compar
ed to the estimated excitation cross sections to obtain the predissociation
yields for selected vibrational levels of the D (1)Pi (+)(u), D' (1)Pi (+)
(u) and D " (1)Pi (+)(u) states. The B' (1)Sigma (+)(u) state is inferred t
o have very significant excitation into the H(1s)+H(2p, 2s) dissociative co
ntinuum.