Vibrational Frequencies calculated at HF/6-31G(2df,p)
| 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' |
4133 |
3742 |
160.17 |
|
|
|
| 2 |
A' |
3659 |
3313 |
98.27 |
|
|
|
| 3 |
A' |
2477 |
2243 |
128.41 |
|
|
|
| 4 |
A' |
1376 |
1246 |
121.11 |
|
|
|
| 5 |
A' |
1166 |
1056 |
84.34 |
|
|
|
| 6 |
A' |
793 |
718 |
48.96 |
|
|
|
| 7 |
A' |
488 |
442 |
13.95 |
|
|
|
| 8 |
A" |
693 |
627 |
71.89 |
|
|
|
| 9 |
A" |
554 |
502 |
0.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7669.5 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 6944.7 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(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.273 |
|
|
|
| 2 |
C |
-0.368 |
|
|
|
| 3 |
O |
-0.516 |
|
|
|
| 4 |
H |
0.246 |
|
|
|
| 5 |
H |
0.366 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.503 |
-0.762 |
0.000 |
1.685 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.253 |
-1.985 |
0.000 |
| y |
-1.985 |
-11.341 |
0.000 |
| z |
0.000 |
0.000 |
-18.274 |
|
| Traceless |
| | x | y | z |
| x |
-2.446 |
-1.985 |
0.000 |
| y |
-1.985 |
6.423 |
0.000 |
| z |
0.000 |
0.000 |
-3.976 |
|
| Polar |
| 3z2-r2 | -7.953 |
| x2-y2 | -5.913 |
| xy | -1.985 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.091 |
0.346 |
0.000 |
| y |
0.346 |
4.961 |
0.000 |
| z |
0.000 |
0.000 |
1.881 |
<r2> (average value of r
2) Å
2
| <r2> |
39.619 |
| (<r2>)1/2 |
6.294 |