Vibrational Frequencies calculated at HF/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' |
3402 |
3057 |
9.21 |
|
|
|
| 2 |
A' |
1496 |
1344 |
35.16 |
|
|
|
| 3 |
A' |
1253 |
1126 |
208.29 |
|
|
|
| 4 |
A' |
810 |
727 |
51.46 |
|
|
|
| 5 |
A' |
498 |
447 |
2.80 |
|
|
|
| 6 |
A' |
305 |
274 |
0.43 |
|
|
|
| 7 |
A" |
1425 |
1280 |
97.14 |
|
|
|
| 8 |
A" |
908 |
816 |
269.22 |
|
|
|
| 9 |
A" |
404 |
363 |
0.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5249.2 cm
-1
Scaled (by 0.8985) Zero Point Vibrational Energy (zpe) 4716.4 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 HF/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.075 |
|
|
|
| 2 |
H |
0.251 |
|
|
|
| 3 |
F |
-0.319 |
|
|
|
| 4 |
Cl |
-0.004 |
|
|
|
| 5 |
Cl |
-0.004 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.346 |
0.733 |
0.000 |
1.533 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.084 |
-2.038 |
-0.001 |
| y |
-2.038 |
-35.875 |
0.003 |
| z |
-0.001 |
0.003 |
-37.007 |
|
| Traceless |
| | x | y | z |
| x |
0.356 |
-2.038 |
-0.001 |
| y |
-2.038 |
0.671 |
0.003 |
| z |
-0.001 |
0.003 |
-1.027 |
|
| Polar |
| 3z2-r2 | -2.054 |
| x2-y2 | -0.209 |
| xy | -2.038 |
| xz | -0.001 |
| yz | 0.003 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.009 |
0.071 |
-0.002 |
| y |
0.071 |
3.854 |
-0.003 |
| z |
-0.002 |
-0.003 |
5.846 |
<r2> (average value of r
2) Å
2
| <r2> |
129.989 |
| (<r2>)1/2 |
11.401 |