The energy of the first excited levels of benzene is calculated by the method of antisymmetrized molecular orbitals. The results predict two weak bands, due to forbidden electronic transitions, at λ = 2500 and λ = 2100 and a strong band at λ = 1500. No empirical data except the carbon‐carbon distance in benzene were used.

1.
A. L.
Sklar
,
J. Chem. Phys.
5
,
669
(
1937
).
2.
R. S.
Mulliken
,
J. Chem. Phys.
1
,
492
(
1933
);
R. S.
Mulliken
,
Phys. Rev.
32
,
186
,
761
(
1928
);
R. S.
Mulliken
,
33
,
730
(
1929
); ,
Phys. Rev.
R. S.
Mulliken
,
40
,
55
, ,
Phys. Rev.
R. S.
Mulliken
,
41
,
49
,
751
; ,
Phys. Rev.
R. S.
Mulliken
,
43
,
279
(
1932–3
). ,
Phys. Rev.
J. E.
Lennard‐Jones
,
Trans. Faraday Soc.
25
,
668
(
1929
).
G.
Herzberg
,
Zeits. f. Physik
57
,
601
(
1929
).
3.
E.
Hückel
,
Zeits. f. Physik
70
,
204
(
1931
).
4.
Bright
Wilson
,
Phys. Rev.
45
,
706
(
1934
).
5.
Mulliken
,
Phys. Rev.
43
,
279
(
1933
).
6.
Zener
,
Phys. Rev.
36
,
51
(
1930
).
7.
Handbuch der Physik, Vol. 24, No. 2, p. 143.
8.
Handbuch der Physik, Vol. 24, No. 1. p. 643.
9.
J. H.
Bartlett
,
Phys. Rev.
37
,
507
(
1931
). In Bartlett’s notation, A = i1+12i7 and C = i2+12i8.
10.
The two parameters are the difference between the Coulomb energy of a polar and a nonpolar state and the resonance integral ∫ψa(1)ψb(2)Hψa*(2). Their values were estimated from the absorption frequency of pentene 2 (since cyclohexene has not been measured), and from the resonance of cyclohexene. States like “see the artwork from the pdf” and “see the artwork from the pdf” were omitted since they introduced new variables and complicated the determinant.
11.
V.
Henri
,
J. de. Phys.
3
,
181
(
1922
).
12.
N.
Chako
,
J. Chem. Phys.
2
,
644
(
1934
).
13.
E. P.
Carr
and
H.
Stücklen
,
J. Chem. Phys.
6
,
55
(
1938
).
This content is only available via PDF.
You do not currently have access to this content.