Vibrational Frequencies calculated at HF/Def2TZVPP
| 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' |
4119 |
3734 |
179.08 |
|
|
|
| 2 |
A' |
3632 |
3292 |
104.79 |
|
|
|
| 3 |
A' |
2445 |
2216 |
170.60 |
|
|
|
| 4 |
A' |
1370 |
1241 |
118.74 |
|
|
|
| 5 |
A' |
1165 |
1056 |
93.41 |
|
|
|
| 6 |
A' |
793 |
719 |
55.44 |
|
|
|
| 7 |
A' |
477 |
432 |
16.97 |
|
|
|
| 8 |
A" |
696 |
631 |
81.66 |
|
|
|
| 9 |
A" |
538 |
488 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7617.6 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 6904.6 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 HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.184 |
|
|
|
| 2 |
C |
-0.260 |
|
|
|
| 3 |
O |
-0.367 |
|
|
|
| 4 |
H |
0.189 |
|
|
|
| 5 |
H |
0.255 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.490 |
-0.799 |
0.000 |
1.691 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.779 |
-2.136 |
0.000 |
| y |
-2.136 |
-11.732 |
0.000 |
| z |
0.000 |
0.000 |
-18.847 |
|
| Traceless |
| | x | y | z |
| x |
-2.489 |
-2.136 |
0.000 |
| y |
-2.136 |
6.581 |
0.000 |
| z |
0.000 |
0.000 |
-4.092 |
|
| Polar |
| 3z2-r2 | -8.184 |
| x2-y2 | -6.047 |
| xy | -2.136 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.618 |
0.294 |
0.000 |
| y |
0.294 |
5.382 |
0.000 |
| z |
0.000 |
0.000 |
2.475 |
<r2> (average value of r
2) Å
2
| <r2> |
39.893 |
| (<r2>)1/2 |
6.316 |