Vibrational Frequencies calculated at B3PW91/aug-cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3852 |
3715 |
60.91 |
|
|
|
| 2 |
A |
3297 |
3180 |
9.76 |
|
|
|
| 3 |
A |
3145 |
3033 |
19.91 |
|
|
|
| 4 |
A |
1463 |
1411 |
9.82 |
|
|
|
| 5 |
A |
1353 |
1305 |
28.29 |
|
|
|
| 6 |
A |
1216 |
1173 |
109.42 |
|
|
|
| 7 |
A |
1046 |
1009 |
40.73 |
|
|
|
| 8 |
A |
519 |
501 |
125.50 |
|
|
|
| 9 |
A |
404 |
390 |
23.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8147.0 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 7858.6 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 B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.646 |
|
|
|
| 2 |
O |
-0.319 |
|
|
|
| 3 |
H |
-0.264 |
|
|
|
| 4 |
H |
-0.200 |
|
|
|
| 5 |
H |
0.137 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.067 |
1.449 |
0.221 |
1.468 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.931 |
2.140 |
-0.609 |
| y |
2.140 |
-11.102 |
-0.020 |
| z |
-0.609 |
-0.020 |
-14.570 |
|
| Traceless |
| | x | y | z |
| x |
0.906 |
2.140 |
-0.609 |
| y |
2.140 |
2.148 |
-0.020 |
| z |
-0.609 |
-0.020 |
-3.054 |
|
| Polar |
| 3z2-r2 | -6.108 |
| x2-y2 | -0.828 |
| xy | 2.140 |
| xz | -0.609 |
| yz | -0.020 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.554 |
0.070 |
0.025 |
| y |
0.070 |
2.939 |
-0.009 |
| z |
0.025 |
-0.009 |
2.870 |
<r2> (average value of r
2) Å
2
| <r2> |
20.766 |
| (<r2>)1/2 |
4.557 |