Vibrational Frequencies calculated at B3LYP/3-21G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
1254 |
1206 |
156.85 |
|
|
|
| 2 |
A1 |
844 |
812 |
78.18 |
|
|
|
| 3 |
A1 |
506 |
487 |
31.15 |
|
|
|
| 4 |
A1 |
354 |
340 |
0.03 |
|
|
|
| 5 |
A2 |
358 |
345 |
0.00 |
|
|
|
| 6 |
B1 |
929 |
894 |
194.95 |
|
|
|
| 7 |
B1 |
491 |
473 |
27.99 |
|
|
|
| 8 |
B2 |
1480 |
1423 |
217.17 |
|
|
|
| 9 |
B2 |
505 |
486 |
33.85 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3360.4 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 3232.7 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.272 |
|
|
|
| 2 |
O |
-0.392 |
|
|
|
| 3 |
O |
-0.392 |
|
|
|
| 4 |
F |
-0.243 |
|
|
|
| 5 |
F |
-0.243 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
-0.926 |
0.926 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.148 |
0.000 |
0.000 |
| y |
0.000 |
-35.481 |
0.000 |
| z |
0.000 |
0.000 |
-33.023 |
|
| Traceless |
| | x | y | z |
| x |
3.105 |
0.000 |
0.000 |
| y |
0.000 |
-3.396 |
0.000 |
| z |
0.000 |
0.000 |
0.291 |
|
| Polar |
| 3z2-r2 | 0.582 |
| x2-y2 | 4.334 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.290 |
0.000 |
0.000 |
| y |
0.000 |
3.129 |
0.000 |
| z |
0.000 |
0.000 |
2.578 |
<r2> (average value of r
2) Å
2
| <r2> |
97.018 |
| (<r2>)1/2 |
9.850 |