Vibrational Frequencies calculated at HSEh1PBE/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' |
3122 |
2969 |
29.11 |
|
|
|
| 2 |
A' |
1538 |
1462 |
0.60 |
|
|
|
| 3 |
A' |
1410 |
1341 |
54.92 |
|
|
|
| 4 |
A' |
1151 |
1095 |
163.36 |
|
|
|
| 5 |
A' |
763 |
725 |
100.53 |
|
|
|
| 6 |
A' |
387 |
368 |
1.47 |
|
|
|
| 7 |
A" |
3198 |
3041 |
17.44 |
|
|
|
| 8 |
A" |
1275 |
1212 |
2.33 |
|
|
|
| 9 |
A" |
1035 |
984 |
0.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6939.1 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 6599.1 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/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.103 |
|
|
|
| 2 |
F |
-0.260 |
|
|
|
| 3 |
Cl |
-0.057 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
| 5 |
H |
0.210 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.820 |
1.731 |
0.000 |
1.916 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.667 |
-1.381 |
0.000 |
| y |
-1.381 |
-22.315 |
0.000 |
| z |
0.000 |
0.000 |
-23.111 |
|
| Traceless |
| | x | y | z |
| x |
-2.954 |
-1.381 |
0.000 |
| y |
-1.381 |
2.074 |
0.000 |
| z |
0.000 |
0.000 |
0.880 |
|
| Polar |
| 3z2-r2 | 1.760 |
| x2-y2 | -3.352 |
| xy | -1.381 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.863 |
0.689 |
0.000 |
| y |
0.689 |
3.966 |
0.000 |
| z |
0.000 |
0.000 |
2.486 |
<r2> (average value of r
2) Å
2
| <r2> |
65.478 |
| (<r2>)1/2 |
8.092 |