Vibrational Frequencies calculated at HF/TZVP
| 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' |
3353 |
3046 |
4.55 |
|
|
|
| 2 |
A' |
1484 |
1349 |
33.88 |
|
|
|
| 3 |
A' |
1242 |
1129 |
237.08 |
|
|
|
| 4 |
A' |
796 |
723 |
52.12 |
|
|
|
| 5 |
A' |
497 |
451 |
2.35 |
|
|
|
| 6 |
A' |
298 |
271 |
0.30 |
|
|
|
| 7 |
A" |
1391 |
1264 |
93.88 |
|
|
|
| 8 |
A" |
891 |
809 |
270.30 |
|
|
|
| 9 |
A" |
404 |
367 |
0.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5178.0 cm
-1
Scaled (by 0.9086) Zero Point Vibrational Energy (zpe) 4704.7 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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.269 |
|
|
|
| 2 |
H |
0.127 |
|
|
|
| 3 |
F |
-0.202 |
|
|
|
| 4 |
Cl |
-0.097 |
|
|
|
| 5 |
Cl |
-0.097 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.391 |
0.679 |
0.000 |
1.547 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.349 |
-2.315 |
0.000 |
| y |
-2.315 |
-36.069 |
0.000 |
| z |
0.000 |
0.000 |
-36.901 |
|
| Traceless |
| | x | y | z |
| x |
0.136 |
-2.315 |
0.000 |
| y |
-2.315 |
0.556 |
0.000 |
| z |
0.000 |
0.000 |
-0.692 |
|
| Polar |
| 3z2-r2 | -1.384 |
| x2-y2 | -0.280 |
| xy | -2.315 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.347 |
0.088 |
0.000 |
| y |
0.088 |
4.177 |
0.000 |
| z |
0.000 |
0.000 |
6.166 |
<r2> (average value of r
2) Å
2
| <r2> |
130.783 |
| (<r2>)1/2 |
11.436 |