Vibrational Frequencies calculated at BLYP/cc-pV(T+d)Z
| 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 |
798 |
794 |
103.91 |
|
|
|
| 2 |
A1 |
506 |
504 |
4.79 |
|
|
|
| 3 |
A1 |
459 |
457 |
13.06 |
|
|
|
| 4 |
A1 |
201 |
201 |
0.80 |
|
|
|
| 5 |
A2 |
406 |
404 |
0.00 |
|
|
|
| 6 |
B1 |
760 |
757 |
164.83 |
|
|
|
| 7 |
B1 |
302 |
301 |
7.75 |
|
|
|
| 8 |
B2 |
696 |
693 |
538.88 |
|
|
|
| 9 |
B2 |
467 |
465 |
0.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2297.0 cm
-1
Scaled (by 0.9958) Zero Point Vibrational Energy (zpe) 2287.3 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 BLYP/cc-pV(T+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.914 |
|
|
|
| 2 |
F |
-0.292 |
|
|
|
| 3 |
F |
-0.292 |
|
|
|
| 4 |
F |
-0.165 |
|
|
|
| 5 |
F |
-0.165 |
|
|
|
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 |
0.709 |
0.709 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.420 |
0.000 |
0.000 |
| y |
0.000 |
-37.243 |
0.000 |
| z |
0.000 |
0.000 |
-30.845 |
|
| Traceless |
| | x | y | z |
| x |
2.624 |
0.000 |
0.000 |
| y |
0.000 |
-6.110 |
0.000 |
| z |
0.000 |
0.000 |
3.486 |
|
| Polar |
| 3z2-r2 | 6.973 |
| x2-y2 | 5.822 |
| 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 |
3.601 |
0.000 |
0.000 |
| y |
0.000 |
4.797 |
0.000 |
| z |
0.000 |
0.000 |
2.974 |
<r2> (average value of r
2) Å
2
| <r2> |
111.091 |
| (<r2>)1/2 |
10.540 |