Vibrational Frequencies calculated at PBE1PBE/6-311G*
| 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 |
2974 |
2850 |
77.68 |
|
|
|
| 2 |
A1 |
1148 |
1100 |
0.59 |
|
|
|
| 3 |
A1 |
637 |
610 |
28.95 |
|
|
|
| 4 |
E |
3040 |
2914 |
58.56 |
|
|
|
| 4 |
E |
3040 |
2914 |
58.55 |
|
|
|
| 5 |
E |
1479 |
1418 |
1.76 |
|
|
|
| 5 |
E |
1479 |
1418 |
1.76 |
|
|
|
| 6 |
E |
447 |
429 |
186.29 |
|
|
|
| 6 |
E |
447 |
429 |
186.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7345.8 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 7041.0 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 PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.493 |
|
|
|
| 2 |
C |
-1.084 |
|
|
|
| 3 |
H |
0.197 |
|
|
|
| 4 |
H |
0.197 |
|
|
|
| 5 |
H |
0.197 |
|
|
|
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 |
-5.481 |
5.481 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.706 |
0.000 |
0.000 |
| y |
0.000 |
-11.706 |
0.000 |
| z |
0.000 |
0.000 |
-1.462 |
|
| Traceless |
| | x | y | z |
| x |
-5.122 |
0.000 |
0.000 |
| y |
0.000 |
-5.122 |
0.000 |
| z |
0.000 |
0.000 |
10.244 |
|
| Polar |
| 3z2-r2 | 20.487 |
| 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 |
4.285 |
0.000 |
0.000 |
| y |
0.000 |
4.286 |
0.000 |
| z |
0.000 |
0.000 |
5.638 |
<r2> (average value of r
2) Å
2
| <r2> |
18.647 |
| (<r2>)1/2 |
4.318 |