Vibrational Frequencies calculated at B3LYPultrafine/aug-cc-pVTZ
| 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 |
3103 |
3002 |
1.05 |
|
|
|
| 2 |
A |
3083 |
2983 |
15.38 |
|
|
|
| 3 |
A |
3014 |
2916 |
5.11 |
|
|
|
| 4 |
A |
1471 |
1423 |
13.69 |
|
|
|
| 5 |
A |
1370 |
1326 |
8.69 |
|
|
|
| 6 |
A |
1330 |
1287 |
2.75 |
|
|
|
| 7 |
A |
864 |
835 |
0.69 |
|
|
|
| 8 |
A |
706 |
683 |
0.51 |
|
|
|
| 9 |
A |
566 |
548 |
34.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7752.9 cm
-1
Scaled (by 0.9675) Zero Point Vibrational Energy (zpe) 7500.9 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 B3LYPultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.623 |
|
|
|
| 2 |
S |
-0.072 |
|
|
|
| 3 |
H |
0.247 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.711 |
-0.000 |
0.062 |
1.712 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.717 |
-0.000 |
0.148 |
| y |
-0.000 |
-21.875 |
0.001 |
| z |
0.148 |
0.001 |
-19.384 |
|
| Traceless |
| | x | y | z |
| x |
0.913 |
-0.000 |
0.148 |
| y |
-0.000 |
-2.325 |
0.001 |
| z |
0.148 |
0.001 |
1.412 |
|
| Polar |
| 3z2-r2 | 2.824 |
| x2-y2 | 2.158 |
| xy | -0.000 |
| xz | 0.148 |
| yz | 0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.464 |
0.000 |
0.016 |
| y |
0.000 |
4.968 |
-0.000 |
| z |
0.016 |
-0.000 |
4.431 |
<r2> (average value of r
2) Å
2
| <r2> |
37.532 |
| (<r2>)1/2 |
6.126 |