Vibrational Frequencies calculated at B3PW91/cc-pVDZ
| 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 |
3144 |
3034 |
3.51 |
|
|
|
| 2 |
A |
3113 |
3004 |
11.75 |
|
|
|
| 3 |
A |
3023 |
2917 |
7.18 |
|
|
|
| 4 |
A |
1439 |
1389 |
15.08 |
|
|
|
| 5 |
A |
1387 |
1339 |
9.36 |
|
|
|
| 6 |
A |
1300 |
1254 |
3.55 |
|
|
|
| 7 |
A |
891 |
860 |
15.83 |
|
|
|
| 8 |
A |
848 |
818 |
1.81 |
|
|
|
| 9 |
A |
730 |
704 |
1.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7937.4 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 7659.5 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 B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.209 |
|
|
|
| 2 |
S |
-0.074 |
|
|
|
| 3 |
H |
0.100 |
|
|
|
| 4 |
H |
0.092 |
|
|
|
| 5 |
H |
0.092 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.674 |
0.000 |
0.094 |
1.677 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.236 |
0.000 |
0.166 |
| y |
0.000 |
-21.255 |
-0.000 |
| z |
0.166 |
-0.000 |
-18.815 |
|
| Traceless |
| | x | y | z |
| x |
0.799 |
0.000 |
0.166 |
| y |
0.000 |
-2.229 |
-0.000 |
| z |
0.166 |
-0.000 |
1.430 |
|
| Polar |
| 3z2-r2 | 2.861 |
| x2-y2 | 2.019 |
| xy | 0.000 |
| xz | 0.166 |
| yz | -0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
37.184 |
| (<r2>)1/2 |
6.098 |