Vibrational Frequencies calculated at PBEPBEultrafine/6-31G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3020 |
2978 |
19.40 |
|
|
|
| 2 |
A' |
1464 |
1444 |
0.63 |
|
|
|
| 3 |
A' |
1290 |
1272 |
54.56 |
|
|
|
| 4 |
A' |
1101 |
1086 |
171.03 |
|
|
|
| 5 |
A' |
607 |
599 |
67.76 |
|
|
|
| 6 |
A' |
296 |
292 |
0.59 |
|
|
|
| 7 |
A" |
3103 |
3060 |
12.10 |
|
|
|
| 8 |
A" |
1212 |
1195 |
1.87 |
|
|
|
| 9 |
A" |
910 |
897 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6501.2 cm
-1
Scaled (by 0.9863) Zero Point Vibrational Energy (zpe) 6412.1 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 PBEPBEultrafine/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.043 |
|
|
|
| 2 |
F |
-0.228 |
|
|
|
| 3 |
Br |
-0.132 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
| 5 |
H |
0.158 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.483 |
-0.902 |
0.000 |
1.736 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.745 |
-2.749 |
0.000 |
| y |
-2.749 |
-28.947 |
0.000 |
| z |
0.000 |
0.000 |
-28.928 |
|
| Traceless |
| | x | y | z |
| x |
0.192 |
-2.749 |
0.000 |
| y |
-2.749 |
-0.110 |
0.000 |
| z |
0.000 |
0.000 |
-0.082 |
|
| Polar |
| 3z2-r2 | -0.165 |
| x2-y2 | 0.201 |
| xy | -2.749 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.583 |
-0.413 |
0.000 |
| y |
-0.413 |
5.746 |
0.000 |
| z |
0.000 |
0.000 |
3.415 |
<r2> (average value of r
2) Å
2
| <r2> |
92.353 |
| (<r2>)1/2 |
9.610 |