Vibrational Frequencies calculated at B3PW91/6-31G*
| 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' |
3180 |
3042 |
8.27 |
|
|
|
| 2 |
A' |
1358 |
1299 |
24.71 |
|
|
|
| 3 |
A' |
1150 |
1100 |
191.15 |
|
|
|
| 4 |
A' |
742 |
709 |
48.73 |
|
|
|
| 5 |
A' |
458 |
438 |
2.31 |
|
|
|
| 6 |
A' |
278 |
266 |
0.24 |
|
|
|
| 7 |
A" |
1291 |
1235 |
67.83 |
|
|
|
| 8 |
A" |
789 |
755 |
278.33 |
|
|
|
| 9 |
A" |
367 |
351 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4805.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 4597.4 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 B3PW91/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.060 |
|
|
|
| 2 |
H |
0.252 |
|
|
|
| 3 |
F |
-0.219 |
|
|
|
| 4 |
Cl |
0.014 |
|
|
|
| 5 |
Cl |
0.014 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.122 |
0.816 |
0.000 |
1.387 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-35.423 |
-1.692 |
0.000 |
| y |
-1.692 |
-35.176 |
0.000 |
| z |
0.000 |
0.000 |
-36.433 |
|
| Traceless |
| | x | y | z |
| x |
0.381 |
-1.692 |
0.000 |
| y |
-1.692 |
0.752 |
0.000 |
| z |
0.000 |
0.000 |
-1.133 |
|
| Polar |
| 3z2-r2 | -2.266 |
| x2-y2 | -0.247 |
| xy | -1.692 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.177 |
0.139 |
0.000 |
| y |
0.139 |
4.115 |
0.000 |
| z |
0.000 |
0.000 |
6.281 |
<r2> (average value of r
2) Å
2
| <r2> |
131.906 |
| (<r2>)1/2 |
11.485 |