Vibrational Frequencies calculated at B3LYP/6-311G*
| 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 |
3159 |
3052 |
10.97 |
|
|
|
| 2 |
A1 |
2952 |
2853 |
220.71 |
|
|
|
| 3 |
A1 |
1533 |
1481 |
4.60 |
|
|
|
| 4 |
A1 |
1250 |
1207 |
24.83 |
|
|
|
| 5 |
A1 |
985 |
951 |
86.81 |
|
|
|
| 6 |
A1 |
763 |
737 |
0.22 |
|
|
|
| 7 |
A1 |
458 |
443 |
19.32 |
|
|
|
| 8 |
A2 |
1412 |
1364 |
0.00 |
|
|
|
| 9 |
A2 |
1263 |
1220 |
0.00 |
|
|
|
| 10 |
A2 |
939 |
907 |
0.00 |
|
|
|
| 11 |
E |
3155 |
3049 |
36.93 |
|
|
|
| 11 |
E |
3155 |
3049 |
36.94 |
|
|
|
| 12 |
E |
2932 |
2833 |
28.80 |
|
|
|
| 12 |
E |
2932 |
2833 |
28.79 |
|
|
|
| 13 |
E |
1515 |
1464 |
2.06 |
|
|
|
| 13 |
E |
1515 |
1464 |
2.06 |
|
|
|
| 14 |
E |
1459 |
1410 |
28.88 |
|
|
|
| 14 |
E |
1459 |
1410 |
28.88 |
|
|
|
| 15 |
E |
1342 |
1297 |
0.64 |
|
|
|
| 15 |
E |
1342 |
1297 |
0.64 |
|
|
|
| 16 |
E |
1193 |
1153 |
208.75 |
|
|
|
| 16 |
E |
1193 |
1153 |
208.75 |
|
|
|
| 17 |
E |
1085 |
1048 |
81.19 |
|
|
|
| 17 |
E |
1085 |
1048 |
81.18 |
|
|
|
| 18 |
E |
952 |
920 |
52.48 |
|
|
|
| 18 |
E |
952 |
920 |
52.49 |
|
|
|
| 19 |
E |
533 |
515 |
7.62 |
|
|
|
| 19 |
E |
533 |
515 |
7.62 |
|
|
|
| 20 |
E |
292 |
282 |
0.14 |
|
|
|
| 20 |
E |
292 |
282 |
0.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21813.5 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 21078.4 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/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.086 |
|
|
|
| 2 |
C |
-0.086 |
|
|
|
| 3 |
C |
-0.086 |
|
|
|
| 4 |
O |
-0.320 |
|
|
|
| 5 |
O |
-0.320 |
|
|
|
| 6 |
O |
-0.320 |
|
|
|
| 7 |
H |
0.225 |
|
|
|
| 8 |
H |
0.181 |
|
|
|
| 9 |
H |
0.225 |
|
|
|
| 10 |
H |
0.181 |
|
|
|
| 11 |
H |
0.225 |
|
|
|
| 12 |
H |
0.181 |
|
|
|
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 |
1.948 |
1.948 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.004 |
0.000 |
2.009 |
2.009 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.004 |
0.000 |
0.000 |
| y |
0.000 |
-35.004 |
0.000 |
| z |
0.000 |
0.000 |
-35.771 |
|
| Traceless |
| | x | y | z |
| x |
0.383 |
0.000 |
0.000 |
| y |
0.000 |
0.383 |
0.000 |
| z |
0.000 |
0.000 |
-0.767 |
|
| Polar |
| 3z2-r2 | -1.533 |
| 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 |
6.389 |
0.000 |
0.000 |
| y |
0.000 |
6.389 |
0.000 |
| z |
0.000 |
0.000 |
5.403 |
<r2> (average value of r
2) Å
2
| <r2> |
126.870 |
| (<r2>)1/2 |
11.264 |