Vibrational Frequencies calculated at HSEh1PBE/3-21G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
3562 |
3432 |
0.00 |
55.71 |
0.18 |
0.31 |
| 2 |
Σg |
2101 |
2023 |
0.00 |
42.46 |
0.29 |
0.46 |
| 3 |
Σu |
3449 |
3322 |
89.06 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
738 |
711 |
0.00 |
2.78 |
0.75 |
0.86 |
| 4 |
Πg |
738 |
711 |
0.00 |
2.78 |
0.75 |
0.86 |
| 5 |
Πu |
800 |
770 |
111.54 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
800 |
770 |
111.54 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 6093.6 cm
-1
Scaled (by 0.9633) Zero Point Vibrational Energy (zpe) 5869.9 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.281 |
|
|
|
| 2 |
C |
-0.281 |
|
|
|
| 3 |
H |
0.281 |
|
|
|
| 4 |
H |
0.281 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.336 |
0.000 |
0.000 |
| y |
0.000 |
-13.336 |
0.000 |
| z |
0.000 |
0.000 |
-6.763 |
|
| Traceless |
| | x | y | z |
| x |
-3.286 |
0.000 |
0.000 |
| y |
0.000 |
-3.286 |
0.000 |
| z |
0.000 |
0.000 |
6.573 |
|
| Polar |
| 3z2-r2 | 13.145 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.849 |
0.000 |
0.000 |
| y |
0.000 |
0.849 |
0.000 |
| z |
0.000 |
0.000 |
3.928 |
<r2> (average value of r
2) Å
2
| <r2> |
16.851 |
| (<r2>)1/2 |
4.105 |