Vibrational Frequencies calculated at HF/6-31G**
| 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' |
4148 |
3744 |
158.86 |
|
|
|
| 2 |
A' |
3664 |
3307 |
96.28 |
|
|
|
| 3 |
A' |
2479 |
2238 |
128.37 |
|
|
|
| 4 |
A' |
1367 |
1234 |
138.76 |
|
|
|
| 5 |
A' |
1171 |
1057 |
87.47 |
|
|
|
| 6 |
A' |
794 |
716 |
50.51 |
|
|
|
| 7 |
A' |
467 |
422 |
14.71 |
|
|
|
| 8 |
A" |
698 |
630 |
75.06 |
|
|
|
| 9 |
A" |
533 |
481 |
2.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7661.0 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 6914.8 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/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.149 |
|
|
|
| 2 |
C |
-0.141 |
|
|
|
| 3 |
O |
-0.613 |
|
|
|
| 4 |
H |
0.229 |
|
|
|
| 5 |
H |
0.376 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.643 |
-0.744 |
0.000 |
1.804 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.424 |
-2.049 |
0.000 |
| y |
-2.049 |
-11.407 |
0.000 |
| z |
0.000 |
0.000 |
-18.321 |
|
| Traceless |
| | x | y | z |
| x |
-2.560 |
-2.049 |
0.000 |
| y |
-2.049 |
6.466 |
0.000 |
| z |
0.000 |
0.000 |
-3.906 |
|
| Polar |
| 3z2-r2 | -7.812 |
| x2-y2 | -6.018 |
| xy | -2.049 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.724 |
0.470 |
0.000 |
| y |
0.470 |
4.918 |
0.000 |
| z |
0.000 |
0.000 |
1.432 |
<r2> (average value of r
2) Å
2
| <r2> |
39.915 |
| (<r2>)1/2 |
6.318 |