Vibrational Frequencies calculated at HF/CEP-121G
| 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' |
3371 |
3076 |
7.49 |
|
|
|
| 2 |
A' |
3233 |
2950 |
12.43 |
|
|
|
| 3 |
A' |
1827 |
1667 |
137.24 |
|
|
|
| 4 |
A' |
1590 |
1451 |
41.35 |
|
|
|
| 5 |
A' |
1342 |
1225 |
13.92 |
|
|
|
| 6 |
A' |
506 |
462 |
92.88 |
|
|
|
| 7 |
A' |
369 |
337 |
1.98 |
|
|
|
| 8 |
A" |
1307 |
1193 |
9.70 |
|
|
|
| 9 |
A" |
543 |
495 |
0.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7044.5 cm
-1
Scaled (by 0.9125) Zero Point Vibrational Energy (zpe) 6428.1 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/CEP-121G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.157 |
|
|
|
| 2 |
C |
0.081 |
|
|
|
| 3 |
H |
0.184 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
| 5 |
O |
-0.286 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
5.524 |
-0.296 |
0.000 |
5.532 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-14.844 |
-0.267 |
0.000 |
| y |
-0.267 |
-17.359 |
0.000 |
| z |
0.000 |
0.000 |
-17.242 |
|
| Traceless |
| | x | y | z |
| x |
2.456 |
-0.267 |
0.000 |
| y |
-0.267 |
-1.316 |
0.000 |
| z |
0.000 |
0.000 |
-1.140 |
|
| Polar |
| 3z2-r2 | -2.280 |
| x2-y2 | 2.515 |
| xy | -0.267 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.603 |
0.440 |
0.000 |
| y |
0.440 |
2.319 |
0.000 |
| z |
0.000 |
0.000 |
1.140 |
<r2> (average value of r
2) Å
2
| <r2> |
34.635 |
| (<r2>)1/2 |
5.885 |