Vibrational Frequencies calculated at B3PW91/cc-pVTZ
| 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 |
741 |
713 |
57.88 |
|
|
|
| 2 |
A1 |
576 |
554 |
1.41 |
|
|
|
| 3 |
A1 |
358 |
344 |
26.95 |
|
|
|
| 4 |
A1 |
164 |
158 |
1.06 |
|
|
|
| 5 |
A2 |
360 |
346 |
0.00 |
|
|
|
| 6 |
B1 |
722 |
694 |
109.63 |
|
|
|
| 7 |
B1 |
240 |
231 |
12.73 |
|
|
|
| 8 |
B2 |
637 |
612 |
337.08 |
|
|
|
| 9 |
B2 |
396 |
381 |
11.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2096.4 cm
-1
Scaled (by 0.9616) Zero Point Vibrational Energy (zpe) 2015.9 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 B3PW91/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
1.158 |
|
|
|
| 2 |
F |
-0.346 |
|
|
|
| 3 |
F |
-0.346 |
|
|
|
| 4 |
F |
-0.233 |
|
|
|
| 5 |
F |
-0.233 |
|
|
|
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 |
1.753 |
1.753 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.829 |
0.000 |
0.000 |
| y |
0.000 |
-43.708 |
0.000 |
| z |
0.000 |
0.000 |
-35.374 |
|
| Traceless |
| | x | y | z |
| x |
2.712 |
0.000 |
0.000 |
| y |
0.000 |
-7.607 |
0.000 |
| z |
0.000 |
0.000 |
4.895 |
|
| Polar |
| 3z2-r2 | 9.789 |
| x2-y2 | 6.879 |
| 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 |
4.033 |
0.000 |
0.000 |
| y |
0.000 |
5.089 |
0.000 |
| z |
0.000 |
0.000 |
3.385 |
<r2> (average value of r
2) Å
2
| <r2> |
125.954 |
| (<r2>)1/2 |
11.223 |