Vibrational Frequencies calculated at HSEh1PBE/3-21G
| 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' |
3229 |
3110 |
2.67 |
|
|
|
| 2 |
A' |
1335 |
1286 |
22.49 |
|
|
|
| 3 |
A' |
1165 |
1122 |
159.17 |
|
|
|
| 4 |
A' |
669 |
645 |
54.88 |
|
|
|
| 5 |
A' |
400 |
385 |
5.53 |
|
|
|
| 6 |
A' |
253 |
243 |
1.12 |
|
|
|
| 7 |
A" |
1245 |
1199 |
61.28 |
|
|
|
| 8 |
A" |
696 |
671 |
274.02 |
|
|
|
| 9 |
A" |
327 |
315 |
0.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4659.1 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 4488.1 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 HSEh1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.244 |
|
|
|
| 2 |
H |
0.330 |
|
|
|
| 3 |
F |
-0.225 |
|
|
|
| 4 |
Cl |
0.070 |
|
|
|
| 5 |
Cl |
0.070 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.311 |
1.293 |
0.000 |
1.841 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-36.054 |
-2.006 |
0.000 |
| y |
-2.006 |
-36.025 |
0.000 |
| z |
0.000 |
0.000 |
-38.649 |
|
| Traceless |
| | x | y | z |
| x |
1.283 |
-2.006 |
0.000 |
| y |
-2.006 |
1.327 |
0.000 |
| z |
0.000 |
0.000 |
-2.610 |
|
| Polar |
| 3z2-r2 | -5.220 |
| x2-y2 | -0.029 |
| xy | -2.006 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.306 |
0.226 |
0.000 |
| y |
0.226 |
3.649 |
0.000 |
| z |
0.000 |
0.000 |
6.295 |
<r2> (average value of r
2) Å
2
| <r2> |
140.117 |
| (<r2>)1/2 |
11.837 |