Vibrational Frequencies calculated at B3LYP/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 |
693 |
675 |
54.87 |
|
|
|
| 2 |
A1 |
493 |
480 |
1.63 |
|
|
|
| 3 |
A1 |
344 |
335 |
29.45 |
|
|
|
| 4 |
A1 |
97 |
94 |
1.14 |
|
|
|
| 5 |
A2 |
326 |
318 |
0.00 |
|
|
|
| 6 |
B1 |
699 |
681 |
107.49 |
|
|
|
| 7 |
B1 |
248 |
242 |
17.11 |
|
|
|
| 8 |
B2 |
734 |
715 |
377.46 |
|
|
|
| 9 |
B2 |
358 |
349 |
3.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1995.4 cm
-1
Scaled (by 0.9745) Zero Point Vibrational Energy (zpe) 1944.5 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/CEP-121G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
1.302 |
|
|
|
| 2 |
F |
-0.383 |
|
|
|
| 3 |
F |
-0.383 |
|
|
|
| 4 |
F |
-0.268 |
|
|
|
| 5 |
F |
-0.268 |
|
|
|
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 |
2.218 |
2.218 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.442 |
0.000 |
0.000 |
| y |
0.000 |
-41.241 |
0.000 |
| z |
0.000 |
0.000 |
-30.226 |
|
| Traceless |
| | x | y | z |
| x |
2.291 |
0.000 |
0.000 |
| y |
0.000 |
-9.407 |
0.000 |
| z |
0.000 |
0.000 |
7.116 |
|
| Polar |
| 3z2-r2 | 14.231 |
| x2-y2 | 7.799 |
| 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 |
4.282 |
0.000 |
0.000 |
| y |
0.000 |
6.025 |
0.000 |
| z |
0.000 |
0.000 |
2.722 |
<r2> (average value of r
2) Å
2
| <r2> |
102.687 |
| (<r2>)1/2 |
10.133 |