Vibrational Frequencies calculated at HF/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 |
3256 |
2958 |
35.28 |
|
|
|
| 2 |
A1 |
1693 |
1538 |
12.50 |
|
|
|
| 3 |
A1 |
1488 |
1352 |
74.63 |
|
|
|
| 4 |
A1 |
964 |
876 |
1.78 |
|
|
|
| 5 |
A2 |
1155 |
1049 |
0.00 |
|
|
|
| 6 |
B1 |
3355 |
3048 |
35.93 |
|
|
|
| 7 |
B1 |
1285 |
1167 |
16.75 |
|
|
|
| 8 |
B2 |
1395 |
1268 |
1.84 |
|
|
|
| 9 |
B2 |
992 |
901 |
36.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7791.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 7078.8 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 HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.263 |
|
|
|
| 2 |
H |
0.100 |
|
|
|
| 3 |
H |
0.100 |
|
|
|
| 4 |
O |
-0.232 |
|
|
|
| 5 |
O |
-0.232 |
|
|
|
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 |
2.929 |
2.929 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.244 |
0.000 |
0.000 |
| y |
0.000 |
-17.895 |
0.000 |
| z |
0.000 |
0.000 |
-15.411 |
|
| Traceless |
| | x | y | z |
| x |
0.409 |
0.000 |
0.000 |
| y |
0.000 |
-2.067 |
0.000 |
| z |
0.000 |
0.000 |
1.659 |
|
| Polar |
| 3z2-r2 | 3.317 |
| x2-y2 | 1.651 |
| 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 |
1.907 |
0.000 |
0.000 |
| y |
0.000 |
2.528 |
0.000 |
| z |
0.000 |
0.000 |
2.698 |
<r2> (average value of r
2) Å
2
| <r2> |
29.577 |
| (<r2>)1/2 |
5.438 |