Vibrational Frequencies calculated at B1B95/6-31G**
| 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' |
3102 |
2962 |
28.19 |
|
|
|
| 2 |
A' |
1519 |
1450 |
0.68 |
|
|
|
| 3 |
A' |
1390 |
1327 |
50.71 |
|
|
|
| 4 |
A' |
1149 |
1097 |
163.61 |
|
|
|
| 5 |
A' |
752 |
718 |
100.58 |
|
|
|
| 6 |
A' |
382 |
365 |
1.50 |
|
|
|
| 7 |
A" |
3181 |
3037 |
16.44 |
|
|
|
| 8 |
A" |
1263 |
1206 |
2.32 |
|
|
|
| 9 |
A" |
1020 |
974 |
0.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6878.3 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 6567.4 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 B1B95/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.002 |
|
|
|
| 2 |
F |
-0.266 |
|
|
|
| 3 |
Cl |
-0.062 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
| 5 |
H |
0.165 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.824 |
1.721 |
0.000 |
1.908 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.583 |
-1.380 |
0.000 |
| y |
-1.380 |
-22.225 |
0.000 |
| z |
0.000 |
0.000 |
-23.018 |
|
| Traceless |
| | x | y | z |
| x |
-2.961 |
-1.380 |
0.000 |
| y |
-1.380 |
2.075 |
0.000 |
| z |
0.000 |
0.000 |
0.886 |
|
| Polar |
| 3z2-r2 | 1.773 |
| x2-y2 | -3.358 |
| xy | -1.380 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.893 |
0.693 |
0.000 |
| y |
0.693 |
3.999 |
0.000 |
| z |
0.000 |
0.000 |
2.509 |
<r2> (average value of r
2) Å
2
| <r2> |
65.391 |
| (<r2>)1/2 |
8.086 |