Vibrational Frequencies calculated at B3PW91/6-31G
| 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 |
3193 |
3058 |
4.90 |
|
|
|
| 2 |
A |
3162 |
3029 |
11.31 |
|
|
|
| 3 |
A |
3064 |
2934 |
6.09 |
|
|
|
| 4 |
A |
1512 |
1448 |
21.52 |
|
|
|
| 5 |
A |
1470 |
1408 |
15.90 |
|
|
|
| 6 |
A |
1389 |
1331 |
3.57 |
|
|
|
| 7 |
A |
940 |
901 |
22.75 |
|
|
|
| 8 |
A |
917 |
879 |
3.65 |
|
|
|
| 9 |
A |
683 |
654 |
0.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8166.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 7820.6 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 B3PW91/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.735 |
|
|
|
| 2 |
S |
0.083 |
|
|
|
| 3 |
H |
0.220 |
|
|
|
| 4 |
H |
0.216 |
|
|
|
| 5 |
H |
0.216 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.981 |
-0.000 |
0.085 |
1.983 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.621 |
-0.000 |
0.162 |
| y |
-0.000 |
-21.563 |
-0.001 |
| z |
0.162 |
-0.001 |
-18.899 |
|
| Traceless |
| | x | y | z |
| x |
0.610 |
-0.000 |
0.162 |
| y |
-0.000 |
-2.303 |
-0.001 |
| z |
0.162 |
-0.001 |
1.693 |
|
| Polar |
| 3z2-r2 | 3.386 |
| x2-y2 | 1.942 |
| xy | -0.000 |
| xz | 0.162 |
| yz | -0.001 |
|
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> |
38.622 |
| (<r2>)1/2 |
6.215 |