Vibrational Frequencies calculated at HF/Def2TZVPP
| 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 |
1416 |
1284 |
228.33 |
|
|
|
| 2 |
A1 |
997 |
904 |
135.00 |
|
|
|
| 3 |
A1 |
629 |
570 |
49.82 |
|
|
|
| 4 |
A1 |
435 |
395 |
0.09 |
|
|
|
| 5 |
A2 |
432 |
392 |
0.00 |
|
|
|
| 6 |
B1 |
1027 |
931 |
297.78 |
|
|
|
| 7 |
B1 |
621 |
562 |
44.48 |
|
|
|
| 8 |
B2 |
1651 |
1496 |
413.74 |
|
|
|
| 9 |
B2 |
615 |
557 |
46.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3911.0 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 3544.9 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 HF/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.451 |
|
|
|
| 2 |
O |
-0.495 |
|
|
|
| 3 |
O |
-0.495 |
|
|
|
| 4 |
F |
-0.231 |
|
|
|
| 5 |
F |
-0.231 |
|
|
|
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 |
-1.500 |
1.500 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.058 |
0.000 |
0.000 |
| y |
0.000 |
-36.335 |
0.000 |
| z |
0.000 |
0.000 |
-33.319 |
|
| Traceless |
| | x | y | z |
| x |
3.769 |
0.000 |
0.000 |
| y |
0.000 |
-4.146 |
0.000 |
| z |
0.000 |
0.000 |
0.377 |
|
| Polar |
| 3z2-r2 | 0.754 |
| x2-y2 | 5.277 |
| 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 |
2.800 |
0.000 |
0.000 |
| y |
0.000 |
3.475 |
0.000 |
| z |
0.000 |
0.000 |
3.022 |
<r2> (average value of r
2) Å
2
| <r2> |
90.372 |
| (<r2>)1/2 |
9.506 |