Vibrational Frequencies calculated at B3LYP/6-31G*
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
3133 |
3008 |
0.00 |
|
|
|
2 |
A1 |
1523 |
1462 |
0.00 |
|
|
|
3 |
A1 |
1097 |
1053 |
0.00 |
|
|
|
4 |
A1 |
1063 |
1021 |
0.00 |
|
|
|
5 |
A1 |
608 |
583 |
0.00 |
|
|
|
6 |
A2 |
3202 |
3075 |
0.00 |
|
|
|
7 |
A2 |
1183 |
1136 |
0.00 |
|
|
|
8 |
A2 |
846 |
812 |
0.00 |
|
|
|
9 |
B1 |
3201 |
3074 |
0.00 |
|
|
|
10 |
B1 |
1195 |
1147 |
0.00 |
|
|
|
11 |
B1 |
1036 |
994 |
0.00 |
|
|
|
12 |
B1 |
292 |
280 |
0.00 |
|
|
|
13 |
B2 |
3131 |
3007 |
41.87 |
|
|
|
14 |
B2 |
1593 |
1530 |
1.67 |
|
|
|
15 |
B2 |
1455 |
1397 |
0.27 |
|
|
|
16 |
B2 |
1027 |
987 |
7.82 |
|
|
|
17 |
B2 |
911 |
875 |
17.63 |
|
|
|
18 |
E |
3215 |
3087 |
29.34 |
|
|
|
18 |
E |
3215 |
3087 |
29.34 |
|
|
|
19 |
E |
3129 |
3005 |
27.37 |
|
|
|
19 |
E |
3129 |
3005 |
27.37 |
|
|
|
20 |
E |
1492 |
1432 |
0.20 |
|
|
|
20 |
E |
1492 |
1432 |
0.20 |
|
|
|
21 |
E |
1193 |
1145 |
2.36 |
|
|
|
21 |
E |
1193 |
1145 |
2.36 |
|
|
|
22 |
E |
1086 |
1042 |
1.76 |
|
|
|
22 |
E |
1086 |
1042 |
1.76 |
|
|
|
23 |
E |
895 |
860 |
4.63 |
|
|
|
23 |
E |
895 |
860 |
4.63 |
|
|
|
24 |
E |
795 |
763 |
0.33 |
|
|
|
24 |
E |
795 |
763 |
0.33 |
|
|
|
25 |
E |
305 |
293 |
0.23 |
|
|
|
25 |
E |
305 |
293 |
0.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 25354.2 cm
-1
Scaled (by 0.9603) Zero Point Vibrational Energy (zpe) 24347.6 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.120 |
0.242 |
|
0.258 |
2 |
C |
-0.328 |
-0.240 |
|
-0.297 |
3 |
C |
-0.328 |
-0.239 |
|
-0.297 |
4 |
C |
-0.328 |
-0.239 |
|
-0.293 |
5 |
C |
-0.328 |
-0.240 |
|
-0.300 |
6 |
H |
0.149 |
0.089 |
|
0.118 |
7 |
H |
0.149 |
0.089 |
|
0.115 |
8 |
H |
0.149 |
0.089 |
|
0.115 |
9 |
H |
0.149 |
0.089 |
|
0.118 |
10 |
H |
0.149 |
0.089 |
|
0.116 |
11 |
H |
0.149 |
0.089 |
|
0.116 |
12 |
H |
0.149 |
0.089 |
|
0.117 |
13 |
H |
0.149 |
0.089 |
|
0.117 |
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
0.000 |
0.000 |
CHELPG |
0.000 |
0.000 |
0.000 |
0.000 |
AIM |
|
|
|
|
ESP |
0.009 |
0.000 |
0.001 |
0.009 |
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.394 |
0.000 |
0.000 |
y |
0.000 |
-30.394 |
0.000 |
z |
0.000 |
0.000 |
-32.273 |
|
Traceless |
| x | y | z |
x |
0.939 |
0.000 |
0.000 |
y |
0.000 |
0.939 |
0.000 |
z |
0.000 |
0.000 |
-1.879 |
|
Polar |
3z2-r2 | -3.757 |
x2-y2 | 0.000 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.906 |
0.000 |
0.000 |
y |
0.000 |
6.906 |
0.000 |
z |
0.000 |
0.000 |
7.948 |
<r2> (average value of r
2) Å
2
<r2> |
111.829 |
(<r2>)1/2 |
10.575 |