Vibrational Frequencies calculated at HSEh1PBE/cc-pVDZ
| 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' |
3142 |
3022 |
4.37 |
|
|
|
| 2 |
A' |
1423 |
1369 |
0.03 |
|
|
|
| 3 |
A' |
1235 |
1188 |
51.90 |
|
|
|
| 4 |
A' |
757 |
728 |
106.81 |
|
|
|
| 5 |
A' |
617 |
593 |
33.82 |
|
|
|
| 6 |
A' |
230 |
221 |
0.21 |
|
|
|
| 7 |
A" |
3235 |
3112 |
0.50 |
|
|
|
| 8 |
A" |
1137 |
1094 |
0.01 |
|
|
|
| 9 |
A" |
847 |
815 |
3.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6310.9 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 6070.5 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-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.166 |
|
|
|
| 2 |
Br |
-0.046 |
|
|
|
| 3 |
Cl |
-0.067 |
|
|
|
| 4 |
H |
0.140 |
|
|
|
| 5 |
H |
0.140 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.865 |
1.355 |
0.000 |
1.608 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-38.694 |
1.192 |
0.000 |
| y |
1.192 |
-34.810 |
0.000 |
| z |
0.000 |
0.000 |
-36.866 |
|
| Traceless |
| | x | y | z |
| x |
-2.856 |
1.192 |
0.000 |
| y |
1.192 |
2.970 |
0.000 |
| z |
0.000 |
0.000 |
-0.114 |
|
| Polar |
| 3z2-r2 | -0.227 |
| x2-y2 | -3.884 |
| xy | 1.192 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.427 |
-1.500 |
0.000 |
| y |
-1.500 |
5.549 |
0.000 |
| z |
0.000 |
0.000 |
3.427 |
<r2> (average value of r
2) Å
2
| <r2> |
147.520 |
| (<r2>)1/2 |
12.146 |