Vibrational Frequencies calculated at B3LYP/SDD
| 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 |
695 |
669 |
59.39 |
|
|
|
| 2 |
A1 |
476 |
458 |
1.62 |
|
|
|
| 3 |
A1 |
352 |
339 |
31.05 |
|
|
|
| 4 |
A1 |
108 |
104 |
1.29 |
|
|
|
| 5 |
A2 |
334 |
321 |
0.00 |
|
|
|
| 6 |
B1 |
692 |
666 |
108.90 |
|
|
|
| 7 |
B1 |
247 |
237 |
19.17 |
|
|
|
| 8 |
B2 |
688 |
661 |
378.69 |
|
|
|
| 9 |
B2 |
370 |
356 |
2.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1980.8 cm
-1
Scaled (by 0.9613) Zero Point Vibrational Energy (zpe) 1904.1 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/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.486 |
|
|
|
| 2 |
F |
-0.421 |
|
|
|
| 3 |
F |
-0.421 |
|
|
|
| 4 |
F |
-0.322 |
|
|
|
| 5 |
F |
-0.322 |
|
|
|
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 |
2.190 |
2.190 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.870 |
0.000 |
0.000 |
| y |
0.000 |
-41.930 |
0.000 |
| z |
0.000 |
0.000 |
-30.834 |
|
| Traceless |
| | x | y | z |
| x |
2.512 |
0.000 |
0.000 |
| y |
0.000 |
-9.577 |
0.000 |
| z |
0.000 |
0.000 |
7.066 |
|
| Polar |
| 3z2-r2 | 14.132 |
| x2-y2 | 8.059 |
| 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 |
3.833 |
0.000 |
0.000 |
| y |
0.000 |
5.715 |
0.000 |
| z |
0.000 |
0.000 |
2.383 |
<r2> (average value of r
2) Å
2
| <r2> |
125.583 |
| (<r2>)1/2 |
11.206 |