Vibrational Frequencies calculated at HSEh1PBE/daug-cc-pVTZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
2982 |
2982 |
70.17 |
|
|
|
| 2 |
A1 |
1082 |
1082 |
0.19 |
|
|
|
| 3 |
A1 |
636 |
636 |
30.94 |
|
|
|
| 4 |
E |
3051 |
3051 |
44.07 |
|
|
|
| 4 |
E |
3051 |
3051 |
44.06 |
|
|
|
| 5 |
E |
1436 |
1436 |
3.60 |
|
|
|
| 5 |
E |
1436 |
1436 |
3.60 |
|
|
|
| 6 |
E |
424 |
424 |
161.23 |
|
|
|
| 6 |
E |
424 |
424 |
161.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7261.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7261.1 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/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.207 |
|
|
|
| 2 |
C |
-0.693 |
|
|
|
| 3 |
H |
0.162 |
|
|
|
| 4 |
H |
0.162 |
|
|
|
| 5 |
H |
0.162 |
|
|
|
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 |
-5.662 |
5.662 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.782 |
0.000 |
0.000 |
| y |
0.000 |
-11.782 |
0.000 |
| z |
0.000 |
0.000 |
-1.795 |
|
| Traceless |
| | x | y | z |
| x |
-4.994 |
0.000 |
0.000 |
| y |
0.000 |
-4.994 |
0.000 |
| z |
0.000 |
0.000 |
9.987 |
|
| Polar |
| 3z2-r2 | 19.974 |
| 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 |
4.922 |
0.000 |
0.000 |
| y |
0.000 |
4.922 |
-0.001 |
| z |
0.000 |
-0.001 |
6.723 |
<r2> (average value of r
2) Å
2
| <r2> |
18.660 |
| (<r2>)1/2 |
4.320 |