Vibrational Frequencies calculated at HF/CEP-121G*
| 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 |
1339 |
1210 |
234.60 |
|
|
|
| 2 |
A1 |
934 |
844 |
144.48 |
|
|
|
| 3 |
A1 |
585 |
529 |
51.16 |
|
|
|
| 4 |
A1 |
405 |
365 |
0.13 |
|
|
|
| 5 |
A2 |
397 |
359 |
0.00 |
|
|
|
| 6 |
B1 |
966 |
873 |
310.69 |
|
|
|
| 7 |
B1 |
576 |
521 |
43.57 |
|
|
|
| 8 |
B2 |
1572 |
1420 |
414.04 |
|
|
|
| 9 |
B2 |
572 |
517 |
50.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3672.7 cm
-1
Scaled (by 0.9034) Zero Point Vibrational Energy (zpe) 3317.9 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/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.316 |
|
|
|
| 2 |
O |
-0.416 |
|
|
|
| 3 |
O |
-0.416 |
|
|
|
| 4 |
F |
-0.242 |
|
|
|
| 5 |
F |
-0.242 |
|
|
|
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 |
-1.221 |
1.221 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.128 |
0.000 |
0.000 |
| y |
0.000 |
-36.246 |
0.000 |
| z |
0.000 |
0.000 |
-33.294 |
|
| Traceless |
| | x | y | z |
| x |
3.642 |
0.000 |
0.000 |
| y |
0.000 |
-4.035 |
0.000 |
| z |
0.000 |
0.000 |
0.393 |
|
| Polar |
| 3z2-r2 | 0.786 |
| x2-y2 | 5.118 |
| 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 |
2.798 |
0.000 |
0.000 |
| y |
0.000 |
3.529 |
0.000 |
| z |
0.000 |
0.000 |
3.032 |
<r2> (average value of r
2) Å
2
| <r2> |
76.387 |
| (<r2>)1/2 |
8.740 |