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' |
3198 |
3060 |
2.89 |
|
|
|
| 2 |
A' |
1479 |
1415 |
0.28 |
|
|
|
| 3 |
A' |
1287 |
1232 |
43.93 |
|
|
|
| 4 |
A' |
690 |
660 |
110.74 |
|
|
|
| 5 |
A' |
587 |
561 |
34.33 |
|
|
|
| 6 |
A' |
223 |
213 |
0.41 |
|
|
|
| 7 |
A" |
3304 |
3160 |
0.08 |
|
|
|
| 8 |
A" |
1169 |
1118 |
0.00 |
|
|
|
| 9 |
A" |
864 |
827 |
6.27 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6400.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 6122.4 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 HSEh1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.707 |
|
|
|
| 2 |
Br |
0.094 |
|
|
|
| 3 |
Cl |
0.048 |
|
|
|
| 4 |
H |
0.283 |
|
|
|
| 5 |
H |
0.283 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.308 |
1.588 |
0.000 |
2.057 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-40.490 |
1.770 |
0.000 |
| y |
1.770 |
-35.187 |
0.000 |
| z |
0.000 |
0.000 |
-37.133 |
|
| Traceless |
| | x | y | z |
| x |
-4.331 |
1.770 |
0.000 |
| y |
1.770 |
3.625 |
0.000 |
| z |
0.000 |
0.000 |
0.705 |
|
| Polar |
| 3z2-r2 | 1.411 |
| x2-y2 | -5.304 |
| xy | 1.770 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.086 |
-1.765 |
0.000 |
| y |
-1.765 |
4.933 |
0.000 |
| z |
0.000 |
0.000 |
2.442 |
<r2> (average value of r
2) Å
2
| <r2> |
152.988 |
| (<r2>)1/2 |
12.369 |