Vibrational Frequencies calculated at B3LYP/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 |
3129 |
3019 |
2.83 |
|
|
|
| 2 |
A |
3099 |
2991 |
13.37 |
|
|
|
| 3 |
A |
3023 |
2917 |
4.35 |
|
|
|
| 4 |
A |
1470 |
1419 |
13.52 |
|
|
|
| 5 |
A |
1398 |
1349 |
8.02 |
|
|
|
| 6 |
A |
1328 |
1281 |
4.20 |
|
|
|
| 7 |
A |
859 |
829 |
1.29 |
|
|
|
| 8 |
A |
792 |
765 |
24.33 |
|
|
|
| 9 |
A |
711 |
686 |
0.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7904.5 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 7627.9 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 B3LYP/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.376 |
|
|
|
| 2 |
S |
-0.106 |
|
|
|
| 3 |
H |
0.168 |
|
|
|
| 4 |
H |
0.157 |
|
|
|
| 5 |
H |
0.157 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.767 |
-0.000 |
0.076 |
1.768 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.186 |
-0.000 |
0.150 |
| y |
-0.000 |
-21.382 |
-0.001 |
| z |
0.150 |
-0.001 |
-18.978 |
|
| Traceless |
| | x | y | z |
| x |
0.994 |
-0.000 |
0.150 |
| y |
-0.000 |
-2.300 |
-0.001 |
| z |
0.150 |
-0.001 |
1.306 |
|
| Polar |
| 3z2-r2 | 2.612 |
| x2-y2 | 2.196 |
| xy | -0.000 |
| xz | 0.150 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.224 |
0.021 |
0.010 |
| y |
0.021 |
3.506 |
-0.004 |
| z |
0.010 |
-0.004 |
3.282 |
<r2> (average value of r
2) Å
2
| <r2> |
37.286 |
| (<r2>)1/2 |
6.106 |