Vibrational Frequencies calculated at PBEPBE/3-21G
| 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 |
1730 |
1714 |
217.77 |
|
|
|
| 2 |
A1 |
791 |
784 |
42.20 |
|
|
|
| 3 |
A1 |
753 |
746 |
1.73 |
|
|
|
| 4 |
A1 |
498 |
493 |
39.78 |
|
|
|
| 5 |
B1 |
692 |
685 |
0.69 |
|
|
|
| 6 |
B1 |
144 |
143 |
30.71 |
|
|
|
| 7 |
B2 |
709 |
702 |
322.99 |
|
|
|
| 8 |
B2 |
591 |
586 |
15.90 |
|
|
|
| 9 |
B2 |
382 |
378 |
56.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3144.4 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 3115.8 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 PBEPBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.647 |
|
|
|
| 2 |
O |
-0.452 |
|
|
|
| 3 |
Mg |
0.845 |
|
|
|
| 4 |
O |
-0.520 |
|
|
|
| 5 |
O |
-0.520 |
|
|
|
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 |
9.252 |
9.252 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.017 |
0.000 |
0.000 |
| y |
0.000 |
-37.235 |
0.000 |
| z |
0.000 |
0.000 |
-19.584 |
|
| Traceless |
| | x | y | z |
| x |
0.392 |
0.000 |
0.000 |
| y |
0.000 |
-13.434 |
0.000 |
| z |
0.000 |
0.000 |
13.042 |
|
| Polar |
| 3z2-r2 | 26.084 |
| x2-y2 | 9.218 |
| 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 |
4.001 |
0.000 |
0.000 |
| y |
0.000 |
4.998 |
0.000 |
| z |
0.000 |
0.000 |
11.531 |
<r2> (average value of r
2) Å
2
| <r2> |
103.269 |
| (<r2>)1/2 |
10.162 |