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' |
3159 |
3015 |
4.44 |
|
|
|
| 2 |
A' |
1464 |
1397 |
0.17 |
|
|
|
| 3 |
A' |
1269 |
1211 |
55.42 |
|
|
|
| 4 |
A' |
759 |
724 |
103.46 |
|
|
|
| 5 |
A' |
618 |
590 |
34.47 |
|
|
|
| 6 |
A' |
234 |
223 |
0.26 |
|
|
|
| 7 |
A" |
3249 |
3101 |
0.18 |
|
|
|
| 8 |
A" |
1170 |
1116 |
0.00 |
|
|
|
| 9 |
A" |
861 |
822 |
3.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6390.9 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 6098.9 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 |
-0.375 |
|
|
|
| 2 |
Br |
-0.075 |
|
|
|
| 3 |
Cl |
0.002 |
|
|
|
| 4 |
H |
0.224 |
|
|
|
| 5 |
H |
0.224 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.938 |
1.414 |
0.000 |
1.697 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-38.954 |
1.271 |
0.000 |
| y |
1.271 |
-34.665 |
0.000 |
| z |
0.000 |
0.000 |
-36.889 |
|
| Traceless |
| | x | y | z |
| x |
-3.177 |
1.271 |
0.000 |
| y |
1.271 |
3.257 |
0.000 |
| z |
0.000 |
0.000 |
-0.079 |
|
| Polar |
| 3z2-r2 | -0.159 |
| x2-y2 | -4.289 |
| xy | 1.271 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.623 |
-1.380 |
0.000 |
| y |
-1.380 |
5.598 |
0.000 |
| z |
0.000 |
0.000 |
3.828 |
<r2> (average value of r
2) Å
2
| <r2> |
146.997 |
| (<r2>)1/2 |
12.124 |