Vibrational Frequencies calculated at BLYP/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 |
2884 |
2889 |
95.56 |
|
|
|
| 2 |
A1 |
1030 |
1032 |
99.87 |
|
|
|
| 3 |
A1 |
609 |
610 |
6.94 |
|
|
|
| 4 |
E |
2948 |
2953 |
37.55 |
|
|
|
| 4 |
E |
2948 |
2953 |
37.54 |
|
|
|
| 5 |
E |
1384 |
1386 |
11.63 |
|
|
|
| 5 |
E |
1384 |
1386 |
11.63 |
|
|
|
| 6 |
E |
432 |
433 |
203.20 |
|
|
|
| 6 |
E |
432 |
433 |
203.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7025.6 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 7036.9 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Li |
0.184 |
|
|
|
| 2 |
C |
-0.163 |
|
|
|
| 3 |
H |
-0.007 |
|
|
|
| 4 |
H |
-0.007 |
|
|
|
| 5 |
H |
-0.007 |
|
|
|
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 |
-4.998 |
4.998 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.313 |
0.000 |
0.000 |
| y |
0.000 |
-12.313 |
0.000 |
| z |
0.000 |
0.000 |
-2.267 |
|
| Traceless |
| | x | y | z |
| x |
-5.023 |
0.000 |
0.000 |
| y |
0.000 |
-5.023 |
0.000 |
| z |
0.000 |
0.000 |
10.046 |
|
| Polar |
| 3z2-r2 | 20.093 |
| 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 |
5.369 |
0.000 |
0.000 |
| y |
0.000 |
5.369 |
0.001 |
| z |
0.000 |
0.001 |
8.375 |
<r2> (average value of r
2) Å
2
| <r2> |
19.403 |
| (<r2>)1/2 |
4.405 |