Vibrational Frequencies calculated at BLYP/6-311+G(3df,2p)
| 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 |
2893 |
2878 |
96.19 |
|
|
|
| 2 |
A1 |
1049 |
1043 |
21.81 |
|
|
|
| 3 |
A1 |
606 |
603 |
14.37 |
|
|
|
| 4 |
E |
2949 |
2933 |
37.83 |
|
|
|
| 4 |
E |
2949 |
2933 |
37.83 |
|
|
|
| 5 |
E |
1414 |
1406 |
4.95 |
|
|
|
| 5 |
E |
1414 |
1406 |
4.95 |
|
|
|
| 6 |
E |
425 |
423 |
164.43 |
|
|
|
| 6 |
E |
425 |
423 |
164.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7062.2 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 7023.3 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 BLYP/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.246 |
|
|
|
| 2 |
C |
-0.609 |
|
|
|
| 3 |
H |
0.121 |
|
|
|
| 4 |
H |
0.121 |
|
|
|
| 5 |
H |
0.121 |
|
|
|
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 |
-5.432 |
5.432 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.250 |
0.000 |
0.000 |
| y |
0.000 |
-12.250 |
0.000 |
| z |
0.000 |
0.000 |
-2.540 |
|
| Traceless |
| | x | y | z |
| x |
-4.855 |
0.000 |
0.000 |
| y |
0.000 |
-4.855 |
0.000 |
| z |
0.000 |
0.000 |
9.710 |
|
| Polar |
| 3z2-r2 | 19.421 |
| 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 |
5.629 |
0.000 |
0.000 |
| y |
0.000 |
5.630 |
0.001 |
| z |
0.000 |
0.001 |
9.088 |
<r2> (average value of r
2) Å
2
| <r2> |
19.219 |
| (<r2>)1/2 |
4.384 |