Vibrational Frequencies calculated at LSDA/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 |
1825 |
1795 |
242.19 |
|
|
|
| 2 |
A1 |
841 |
827 |
34.83 |
|
|
|
| 3 |
A1 |
808 |
795 |
25.83 |
|
|
|
| 4 |
A1 |
529 |
520 |
51.08 |
|
|
|
| 5 |
B1 |
740 |
728 |
6.06 |
|
|
|
| 6 |
B1 |
167 |
164 |
38.72 |
|
|
|
| 7 |
B2 |
860 |
846 |
332.35 |
|
|
|
| 8 |
B2 |
651 |
640 |
16.75 |
|
|
|
| 9 |
B2 |
474 |
466 |
8.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3447.5 cm
-1
Scaled (by 0.9836) Zero Point Vibrational Energy (zpe) 3391.0 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.626 |
|
|
|
| 2 |
O |
-0.444 |
|
|
|
| 3 |
Mg |
0.686 |
|
|
|
| 4 |
O |
-0.434 |
|
|
|
| 5 |
O |
-0.434 |
|
|
|
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 |
9.351 |
9.351 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.753 |
0.000 |
0.000 |
| y |
0.000 |
-36.894 |
0.000 |
| z |
0.000 |
0.000 |
-18.453 |
|
| Traceless |
| | x | y | z |
| x |
-0.079 |
0.000 |
0.000 |
| y |
0.000 |
-13.791 |
0.000 |
| z |
0.000 |
0.000 |
13.870 |
|
| Polar |
| 3z2-r2 | 27.740 |
| x2-y2 | 9.141 |
| 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 |
3.402 |
0.000 |
0.000 |
| y |
0.000 |
4.527 |
0.000 |
| z |
0.000 |
0.000 |
10.069 |
<r2> (average value of r
2) Å
2
| <r2> |
99.402 |
| (<r2>)1/2 |
9.970 |