Vibrational Frequencies calculated at LSDA/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 |
1823 |
1794 |
261.96 |
|
|
|
| 2 |
A1 |
914 |
899 |
43.80 |
|
|
|
| 3 |
A1 |
819 |
806 |
6.10 |
|
|
|
| 4 |
A1 |
532 |
523 |
60.40 |
|
|
|
| 5 |
B1 |
777 |
765 |
5.99 |
|
|
|
| 6 |
B1 |
165 |
162 |
34.82 |
|
|
|
| 7 |
B2 |
967 |
952 |
527.06 |
|
|
|
| 8 |
B2 |
666 |
655 |
5.32 |
|
|
|
| 9 |
B2 |
438 |
431 |
10.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3550.6 cm
-1
Scaled (by 0.984) Zero Point Vibrational Energy (zpe) 3493.8 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 LSDA/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.466 |
|
|
|
| 2 |
O |
-0.325 |
|
|
|
| 3 |
Mg |
0.713 |
|
|
|
| 4 |
O |
-0.427 |
|
|
|
| 5 |
O |
-0.427 |
|
|
|
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 |
10.066 |
10.066 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.563 |
0.000 |
0.000 |
| y |
0.000 |
-36.042 |
0.000 |
| z |
0.000 |
0.000 |
-17.846 |
|
| Traceless |
| | x | y | z |
| x |
-0.619 |
0.000 |
0.000 |
| y |
0.000 |
-13.338 |
0.000 |
| z |
0.000 |
0.000 |
13.957 |
|
| Polar |
| 3z2-r2 | 27.913 |
| x2-y2 | 8.479 |
| 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 |
4.216 |
0.000 |
0.000 |
| y |
0.000 |
5.208 |
0.000 |
| z |
0.000 |
0.000 |
10.253 |
<r2> (average value of r
2) Å
2
| <r2> |
96.586 |
| (<r2>)1/2 |
9.828 |