Vibrational Frequencies calculated at HF/Def2TZVPP
| 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' |
3335 |
3023 |
3.85 |
|
|
|
| 2 |
A' |
1477 |
1339 |
21.78 |
|
|
|
| 3 |
A' |
1236 |
1121 |
210.36 |
|
|
|
| 4 |
A' |
798 |
724 |
45.22 |
|
|
|
| 5 |
A' |
498 |
451 |
1.56 |
|
|
|
| 6 |
A' |
299 |
271 |
0.14 |
|
|
|
| 7 |
A" |
1389 |
1259 |
73.02 |
|
|
|
| 8 |
A" |
892 |
809 |
253.72 |
|
|
|
| 9 |
A" |
403 |
365 |
0.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5163.8 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 4680.4 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.295 |
|
|
|
| 2 |
H |
0.082 |
|
|
|
| 3 |
F |
-0.216 |
|
|
|
| 4 |
Cl |
-0.081 |
|
|
|
| 5 |
Cl |
-0.081 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.261 |
0.620 |
0.000 |
1.405 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.133 |
-2.142 |
0.000 |
| y |
-2.142 |
-35.781 |
0.000 |
| z |
0.000 |
0.000 |
-36.481 |
|
| Traceless |
| | x | y | z |
| x |
-0.002 |
-2.142 |
0.000 |
| y |
-2.142 |
0.526 |
0.000 |
| z |
0.000 |
0.000 |
-0.524 |
|
| Polar |
| 3z2-r2 | -1.048 |
| x2-y2 | -0.352 |
| xy | -2.142 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.054 |
0.117 |
0.000 |
| y |
0.117 |
4.765 |
0.000 |
| z |
0.000 |
0.000 |
6.665 |
<r2> (average value of r
2) Å
2
| <r2> |
129.393 |
| (<r2>)1/2 |
11.375 |