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One Open Shell

Given are term symbols (up to indices depending on actual case and group) and $ a$ mathend000# and $ b$ mathend000# coefficients. $ n$ mathend000# is the number of electrons in an irrep with degeneracy $ n_{ir}$ mathend000#. Note that not all cases are Roothaan cases.

All single electron cases are described by:

$ a = b = 0$ mathend000#

$ n_{ir}$ mathend000#=2: e (div. groups), $ \pi$ mathend000#, $ \delta$ mathend000# ( $ C_{\infty v}$ mathend000#, $ D_{\infty h}$ mathend000#)
$ n$ mathend000# $ f$ mathend000# e$ ^n$ mathend000# $ \pi^n$ mathend000# $ \delta^n$ mathend000# $ a$ mathend000# $ b$ mathend000#
$ ^3$ mathend000#A $ ^3\Sigma$ mathend000# $ ^3\Sigma$ mathend000# 1 2
2 $ 1/2$ mathend000# $ ^1$ mathend000#E% latex2html id marker 46156
\setcounter{footnote}{1}\fnsymbol{footnote} $ ^1\Delta$ mathend000# $ ^1\Gamma$ mathend000# $ 1/2$ mathend000# 0
$ ^1$ mathend000#A $ ^1\Sigma$ mathend000# $ ^1\Sigma$ mathend000# 0 $ -$ mathend000#2
3 $ 3/4$ mathend000# $ ^2$ mathend000#E $ ^2\Pi$ mathend000# $ ^2\Delta$ mathend000# $ 8/9$ mathend000# $ 8/9$ mathend000#
1 $ n_{ir}$ mathend000#=3: p (O(3)), t ($ T$ mathend000#, $ O$ mathend000#, $ I$ mathend000#)% latex2html id marker 46191
\setcounter{footnote}{2}\fnsymbol{footnote}
$ n$ mathend000# $ f$ mathend000# p$ ^n$ mathend000# $ a$ mathend000# $ b$ mathend000#
$ ^3$ mathend000#P $ 3/4$ mathend000# $ 3/2$ mathend000#
2 $ 1/3$ mathend000# $ ^1$ mathend000#D% latex2html id marker 46212
\setcounter{footnote}{7}\fnsymbol{footnote} $ 9/20$ mathend000# $ -$ mathend000#$ 3/10$ mathend000#
$ ^1$ mathend000#S 0 $ -$ mathend000#$ 3$ mathend000#
$ ^4$ mathend000#S 1 2
3 $ 1/2$ mathend000# $ ^2$ mathend000#D% latex2html id marker 46231
\setcounter{footnote}{7}\fnsymbol{footnote} $ 4/5$ mathend000# $ 4/5$ mathend000#
$ ^2$ mathend000#P $ 2/3$ mathend000# 0
$ ^3$ mathend000#P $ 15/16$ mathend000# $ 9/8$ mathend000#
4 $ 2/3$ mathend000# $ ^1$ mathend000#D% latex2html id marker 46250
\setcounter{footnote}{7}\fnsymbol{footnote} $ 69/80$ mathend000# $ 27/40$ mathend000#
$ ^1$ mathend000#S $ 3/4$ mathend000# 0
5 $ 5/6$ mathend000# $ ^2$ mathend000#P $ 24/25$ mathend000# $ 24/25$ mathend000#
only irrep g($ I$ mathend000#)
(mainly high spin available)
$ n$ mathend000# $ f$ mathend000# g$ ^n$ mathend000# $ a$ mathend000# $ b$ mathend000#
1 $ 1/8$ mathend000# $ ^2$ mathend000#G 0 mathend000# 0 mathend000#
2 $ 1/4$ mathend000# % latex2html id marker 46287
\setcounter{footnote}{8}\fnsymbol{footnote} $ 2/3$ mathend000# $ 4/3$ mathend000#
$ ^1$ mathend000#A 0 mathend000# $ -$ mathend000#$ 4$ mathend000#
3 $ 3/8$ mathend000# $ ^4$ mathend000#G $ 8/9$ mathend000# $ 16/9$ mathend000#
4 $ 1/2$ mathend000# $ ^5$ mathend000#A $ 1$ mathend000# $ 2$ mathend000#
5 $ 5/8$ mathend000# $ ^4$ mathend000#G$ 24/25$ mathend000#$ 32/25$ mathend000#
6 $ 3/4$ mathend000# % latex2html id marker 46325
\setcounter{footnote}{8}\fnsymbol{footnote}$ 26/27$ mathend000#$ 28/27$ mathend000#
$ ^1$ mathend000#A $ 8/9$ mathend000# $ 4/9$ mathend000#
7 $ 7/8$ mathend000# $ ^2$ mathend000#G$ 48/49$ mathend000#$ 48/49$ mathend000#
d(O3), h($ I$ mathend000#)
(mainly high-spin cases work)
$ n$ mathend000# $ f$ mathend000# d$ ^n$ mathend000# $ a$ mathend000# $ b$ mathend000#
1 $ 1/10$ mathend000# $ ^2$ mathend000#D 0 mathend000# 0 mathend000#
2 $ 1/5$ mathend000# $ ^3$ mathend000#F$ + ^3$ mathend000#P% latex2html id marker 46368
\setcounter{footnote}{8}\fnsymbol{footnote} $ 5/8$ mathend000# $ 5/4$ mathend000#
$ ^1$ mathend000#S 0 mathend000# $ -$ mathend000#$ 5$ mathend000#
3 $ 3/10$ mathend000# $ ^4$ mathend000#F$ + ^4$ mathend000#P% latex2html id marker 46386
\setcounter{footnote}{8}\fnsymbol{footnote} $ 5/6$ mathend000# $ 5/3$ mathend000#
4 $ 2/5$ mathend000# $ ^5$ mathend000#D, $ ^5$ mathend000#H $ 15/16$ mathend000# $ 15/8$ mathend000#
5 $ 1/2$ mathend000# $ ^6$ mathend000#S, $ ^6$ mathend000#A $ 1$ mathend000# $ 2$ mathend000#
6 $ 3/5$ mathend000# $ ^5$ mathend000#D, $ ^5$ mathend000#H $ 35/36$ mathend000# $ 25/18$ mathend000#
7 $ 7/10$ mathend000# $ ^4$ mathend000#F$ + ^4$ mathend000#P% latex2html id marker 46427
\setcounter{footnote}{8}\fnsymbol{footnote} $ 95/98$ mathend000# $ 55/49$ mathend000#
8 $ 4/5$ mathend000# $ ^3$ mathend000#F$ + ^3$ mathend000#P% latex2html id marker 46438
\setcounter{footnote}{8}\fnsymbol{footnote}$ 125/128$ mathend000# $ 65/64$ mathend000#
$ ^1$ mathend000#S $ 15/16$ mathend000# $ 5/8$ mathend000#
9 $ 9/10$ mathend000# $ ^2$ mathend000#D, $ ^2$ mathend000#H $ 80/81$ mathend000# $ 80/81$ mathend000#
    % latex2html id marker 46459
\setcounter{footnote}{1}\fnsymbol{footnote}except cases (e.g. $ D_{2d}$ mathend000# or $ D_{4h}$ mathend000#) where $ \rm e^2$ mathend000# gives only one-dimensional irreps, which are not Roothaan cases.
    % latex2html id marker 46466
\setcounter{footnote}{2}\fnsymbol{footnote}only p$ ^n$ mathend000# given, the state for groups $ T_d$ mathend000# etc. follows from
S $ \rightarrow$ mathend000# A ($ T$ mathend000#,$ O$ mathend000#,$ I$ mathend000#) P $ \rightarrow$ mathend000# T ($ T$ mathend000#,$ O$ mathend000#,$ I$ mathend000#) D $ \rightarrow$ mathend000# H ($ I$ mathend000#), E+T ($ T$ mathend000#,$ O$ mathend000#)
    % latex2html id marker 46495
\setcounter{footnote}{7}\fnsymbol{footnote}This is not a CSF in $ T$ mathend000# or $ O$ mathend000#, ($ a,b$ mathend000#) describes average of states resulting from E+T
    % latex2html id marker 46502
\setcounter{footnote}{8}\fnsymbol{footnote}($ a,b$ mathend000#) describes weighted average of high spin states, not a CSF.



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