Vibrational Frequencies calculated at B1B95/STO-3G
| 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 |
3643 |
3217 |
23.22 |
|
|
|
| 2 |
A |
1321 |
1166 |
13.03 |
|
|
|
| 3 |
A |
1024 |
904 |
16.96 |
|
|
|
| 4 |
A |
734 |
648 |
34.73 |
|
|
|
| 5 |
A |
584 |
516 |
33.03 |
|
|
|
| 6 |
A |
451 |
398 |
54.67 |
|
|
|
| 7 |
A |
314 |
278 |
12.00 |
|
|
|
| 8 |
A |
252 |
222 |
3.40 |
|
|
|
| 9 |
A |
223 |
197 |
7.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4272.3 cm
-1
Scaled (by 0.883) Zero Point Vibrational Energy (zpe) 3772.4 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 B1B95/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.601 |
|
|
|
| 2 |
O |
-0.283 |
|
|
|
| 3 |
O |
-0.352 |
|
|
|
| 4 |
O |
-0.130 |
|
|
|
| 5 |
H |
0.163 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.052 |
-0.285 |
0.698 |
0.756 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.427 |
-0.615 |
-1.413 |
| y |
-0.615 |
-29.361 |
1.143 |
| z |
-1.413 |
1.143 |
-23.556 |
|
| Traceless |
| | x | y | z |
| x |
1.031 |
-0.615 |
-1.413 |
| y |
-0.615 |
-4.870 |
1.143 |
| z |
-1.413 |
1.143 |
3.838 |
|
| Polar |
| 3z2-r2 | 7.677 |
| x2-y2 | 3.934 |
| xy | -0.615 |
| xz | -1.413 |
| yz | 1.143 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.203 |
0.146 |
-0.292 |
| y |
0.146 |
2.731 |
-0.075 |
| z |
-0.292 |
-0.075 |
1.435 |
<r2> (average value of r
2) Å
2
| <r2> |
82.204 |
| (<r2>)1/2 |
9.067 |