Abstract
10. The system
1
K → 2
1
S. A strong system,
v
e
= 21427. In the description of this system is included a rather full account of the manner in which the data for the rotational energy interval tables are obtained and set out. This is generally applicable to similar tables in Parts II-IV . 11. The system
2
L.→2
1
S. This is a very similar system to the preceding but weaker,
v
e
= 23057. 12. The system
1
M → 2
1
S . Strength intermediate between the two preceding systems. Similar in many ways lint differentiated by a change of structure of rotational terms with vibrational energy of initial state,
v
e
= 23191. 13. The system
1
N → 2
1
S. A strong system but has only two progressions,
n
' = 0 and 1. General type similar to preceding three
v
e
= 24896.
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