Vibrational Frequencies calculated at BLYP/6-31G(2df,p)
| 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 |
2906 |
2890 |
67.45 |
|
|
|
| 2 |
A1 |
1054 |
1049 |
105.74 |
|
|
|
| 3 |
A1 |
618 |
615 |
2.95 |
|
|
|
| 4 |
E |
2970 |
2953 |
32.15 |
|
|
|
| 4 |
E |
2970 |
2953 |
32.13 |
|
|
|
| 5 |
E |
1416 |
1408 |
14.49 |
|
|
|
| 5 |
E |
1416 |
1408 |
14.49 |
|
|
|
| 6 |
E |
452 |
449 |
220.90 |
|
|
|
| 6 |
E |
452 |
449 |
220.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7126.5 cm
-1
Scaled (by 0.9945) Zero Point Vibrational Energy (zpe) 7087.3 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.110 |
|
|
|
| 2 |
C |
-0.355 |
|
|
|
| 3 |
H |
0.082 |
|
|
|
| 4 |
H |
0.082 |
|
|
|
| 5 |
H |
0.082 |
|
|
|
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 |
-4.721 |
4.721 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.115 |
0.000 |
0.000 |
| y |
0.000 |
-12.115 |
0.000 |
| z |
0.000 |
0.000 |
-2.441 |
|
| Traceless |
| | x | y | z |
| x |
-4.837 |
0.000 |
0.000 |
| y |
0.000 |
-4.837 |
0.000 |
| z |
0.000 |
0.000 |
9.674 |
|
| Polar |
| 3z2-r2 | 19.347 |
| 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 |
5.308 |
0.000 |
0.000 |
| y |
0.000 |
5.308 |
0.001 |
| z |
0.000 |
0.001 |
8.738 |
<r2> (average value of r
2) Å
2
| <r2> |
19.113 |
| (<r2>)1/2 |
4.372 |