Vibrational Frequencies calculated at B3LYP/6-31+G**
| 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 |
2867 |
103.54 |
|
|
|
| 2 |
A1 |
1095 |
1056 |
3.13 |
|
|
|
| 3 |
A1 |
626 |
604 |
26.16 |
|
|
|
| 4 |
E |
3044 |
2935 |
44.90 |
|
|
|
| 4 |
E |
3044 |
2935 |
44.89 |
|
|
|
| 5 |
E |
1456 |
1404 |
1.27 |
|
|
|
| 5 |
E |
1456 |
1404 |
1.27 |
|
|
|
| 6 |
E |
467 |
450 |
166.42 |
|
|
|
| 6 |
E |
467 |
450 |
166.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7314.5 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 7052.6 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 B3LYP/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.321 |
|
|
|
| 2 |
C |
-0.662 |
|
|
|
| 3 |
H |
0.114 |
|
|
|
| 4 |
H |
0.114 |
|
|
|
| 5 |
H |
0.114 |
|
|
|
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 |
-5.529 |
5.529 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.151 |
0.000 |
0.000 |
| y |
0.000 |
-12.151 |
0.000 |
| z |
0.000 |
0.000 |
-2.040 |
|
| Traceless |
| | x | y | z |
| x |
-5.056 |
0.000 |
0.000 |
| y |
0.000 |
-5.056 |
0.000 |
| z |
0.000 |
0.000 |
10.111 |
|
| Polar |
| 3z2-r2 | 20.223 |
| 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 |
4.853 |
0.000 |
0.000 |
| y |
0.000 |
4.854 |
0.001 |
| z |
0.000 |
0.001 |
7.368 |
<r2> (average value of r
2) Å
2
| <r2> |
19.100 |
| (<r2>)1/2 |
4.370 |