Vibrational Frequencies calculated at B3LYP/daug-cc-pVDZ
| 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 |
2958 |
2958 |
86.00 |
|
|
|
| 2 |
A1 |
1070 |
1070 |
4.34 |
|
|
|
| 3 |
A1 |
619 |
619 |
26.21 |
|
|
|
| 4 |
E |
3024 |
3024 |
47.81 |
|
|
|
| 4 |
E |
3024 |
3024 |
47.80 |
|
|
|
| 5 |
E |
1411 |
1411 |
4.61 |
|
|
|
| 5 |
E |
1411 |
1411 |
4.61 |
|
|
|
| 6 |
E |
401 |
401 |
157.55 |
|
|
|
| 6 |
E |
401 |
401 |
157.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7159.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7159.8 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/daug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
-0.368 |
|
|
|
| 2 |
C |
0.717 |
|
|
|
| 3 |
H |
-0.116 |
|
|
|
| 4 |
H |
-0.116 |
|
|
|
| 5 |
H |
-0.116 |
|
|
|
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 |
-5.638 |
5.638 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.113 |
0.000 |
0.000 |
| y |
0.000 |
-12.113 |
0.000 |
| z |
0.000 |
0.000 |
-1.946 |
|
| Traceless |
| | x | y | z |
| x |
-5.083 |
0.000 |
0.000 |
| y |
0.000 |
-5.083 |
0.000 |
| z |
0.000 |
0.000 |
10.167 |
|
| Polar |
| 3z2-r2 | 20.333 |
| 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 |
5.203 |
0.000 |
0.000 |
| y |
0.000 |
5.204 |
0.001 |
| z |
0.000 |
0.001 |
7.467 |
<r2> (average value of r
2) Å
2
| <r2> |
19.026 |
| (<r2>)1/2 |
4.362 |