Vibrational Frequencies calculated at HSEh1PBE/cc-pVTZ
| 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' |
3141 |
3019 |
16.71 |
|
|
|
| 2 |
A' |
1327 |
1275 |
62.84 |
|
|
|
| 3 |
A' |
1138 |
1094 |
229.89 |
|
|
|
| 4 |
A' |
807 |
776 |
159.39 |
|
|
|
| 5 |
A' |
606 |
582 |
6.86 |
|
|
|
| 6 |
A' |
413 |
397 |
0.12 |
|
|
|
| 7 |
A" |
1379 |
1325 |
17.24 |
|
|
|
| 8 |
A" |
1165 |
1120 |
230.18 |
|
|
|
| 9 |
A" |
367 |
353 |
0.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5171.5 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 4970.3 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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.353 |
|
|
|
| 2 |
H |
0.061 |
|
|
|
| 3 |
Cl |
-0.123 |
|
|
|
| 4 |
F |
-0.145 |
|
|
|
| 5 |
F |
-0.145 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.149 |
0.817 |
0.000 |
1.409 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.169 |
-0.990 |
0.000 |
| y |
-0.990 |
-28.905 |
0.000 |
| z |
0.000 |
0.000 |
-29.770 |
|
| Traceless |
| | x | y | z |
| x |
3.169 |
-0.990 |
0.000 |
| y |
-0.990 |
-0.936 |
0.000 |
| z |
0.000 |
0.000 |
-2.233 |
|
| Polar |
| 3z2-r2 | -4.466 |
| x2-y2 | 2.736 |
| xy | -0.990 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.159 |
0.859 |
0.000 |
| y |
0.859 |
3.818 |
0.000 |
| z |
0.000 |
0.000 |
3.267 |
<r2> (average value of r
2) Å
2
| <r2> |
90.325 |
| (<r2>)1/2 |
9.504 |