Vibrational Frequencies calculated at LSDA/6-31+G**
| 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 |
2968 |
2924 |
34.27 |
|
|
|
| 2 |
A1 |
1419 |
1398 |
0.69 |
|
|
|
| 3 |
A1 |
1087 |
1071 |
110.94 |
|
|
|
| 4 |
E |
3065 |
3019 |
22.89 |
|
|
|
| 4 |
E |
3065 |
3019 |
22.89 |
|
|
|
| 5 |
E |
1426 |
1404 |
7.80 |
|
|
|
| 5 |
E |
1426 |
1404 |
7.80 |
|
|
|
| 6 |
E |
1147 |
1130 |
0.01 |
|
|
|
| 6 |
E |
1147 |
1130 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8375.1 cm
-1
Scaled (by 0.985) Zero Point Vibrational Energy (zpe) 8249.5 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 LSDA/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.259 |
|
|
|
| 2 |
F |
-0.281 |
|
|
|
| 3 |
H |
0.180 |
|
|
|
| 4 |
H |
0.180 |
|
|
|
| 5 |
H |
0.180 |
|
|
|
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 |
-1.946 |
1.946 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.090 |
0.000 |
0.000 |
| y |
0.000 |
-12.090 |
0.000 |
| z |
0.000 |
0.000 |
-12.814 |
|
| Traceless |
| | x | y | z |
| x |
0.362 |
0.000 |
0.000 |
| y |
0.000 |
0.362 |
0.000 |
| z |
0.000 |
0.000 |
-0.724 |
|
| Polar |
| 3z2-r2 | -1.447 |
| x2-y2 | 0.000 |
| 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 |
2.214 |
0.000 |
0.000 |
| y |
0.000 |
2.214 |
0.000 |
| z |
0.000 |
0.000 |
2.291 |
<r2> (average value of r
2) Å
2
| <r2> |
21.342 |
| (<r2>)1/2 |
4.620 |