Vibrational Frequencies calculated at B3PW91/6-31+G**
| 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 |
3423 |
3286 |
2.94 |
|
|
|
| 2 |
A1 |
1843 |
1769 |
2.55 |
|
|
|
| 3 |
A1 |
1087 |
1044 |
14.79 |
|
|
|
| 4 |
A1 |
899 |
863 |
59.92 |
|
|
|
| 5 |
A2 |
628 |
603 |
0.00 |
|
|
|
| 6 |
B1 |
545 |
524 |
101.52 |
|
|
|
| 7 |
B2 |
3350 |
3216 |
53.92 |
|
|
|
| 8 |
B2 |
958 |
920 |
6.40 |
|
|
|
| 9 |
B2 |
60i |
57i |
4.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6336.5 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 6083.7 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 B3PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.364 |
|
|
|
| 2 |
C |
-0.024 |
|
|
|
| 3 |
C |
-0.024 |
|
|
|
| 4 |
H |
0.206 |
|
|
|
| 5 |
H |
0.206 |
|
|
|
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 |
-2.599 |
2.599 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.875 |
0.000 |
0.000 |
| y |
0.000 |
-11.570 |
0.000 |
| z |
0.000 |
0.000 |
-19.113 |
|
| Traceless |
| | x | y | z |
| x |
-3.534 |
0.000 |
0.000 |
| y |
0.000 |
7.425 |
0.000 |
| z |
0.000 |
0.000 |
-3.891 |
|
| Polar |
| 3z2-r2 | -7.781 |
| x2-y2 | -7.306 |
| 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 |
2.538 |
0.000 |
0.000 |
| y |
0.000 |
4.670 |
0.000 |
| z |
0.000 |
0.000 |
3.449 |
<r2> (average value of r
2) Å
2
| <r2> |
30.773 |
| (<r2>)1/2 |
5.547 |