Vibrational Frequencies calculated at HF/CEP-31G
| 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 |
1849 |
1666 |
687.46 |
|
|
|
| 2 |
A1 |
962 |
867 |
99.97 |
|
|
|
| 3 |
A1 |
833 |
751 |
30.72 |
|
|
|
| 4 |
A1 |
529 |
477 |
123.30 |
|
|
|
| 5 |
B1 |
835 |
752 |
80.35 |
|
|
|
| 6 |
B1 |
176 |
158 |
63.80 |
|
|
|
| 7 |
B2 |
1153 |
1039 |
657.07 |
|
|
|
| 8 |
B2 |
724 |
653 |
3.79 |
|
|
|
| 9 |
B2 |
504 |
454 |
12.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3781.6 cm
-1
Scaled (by 0.9014) Zero Point Vibrational Energy (zpe) 3408.7 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 HF/CEP-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.419 |
|
|
|
| 2 |
O |
-0.240 |
|
|
|
| 3 |
Mg |
1.354 |
|
|
|
| 4 |
O |
-0.767 |
|
|
|
| 5 |
O |
-0.767 |
|
|
|
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 |
14.300 |
14.300 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.392 |
0.000 |
0.000 |
| y |
0.000 |
-38.927 |
0.000 |
| z |
0.000 |
0.000 |
-13.752 |
|
| Traceless |
| | x | y | z |
| x |
0.948 |
0.000 |
0.000 |
| y |
0.000 |
-19.355 |
0.000 |
| z |
0.000 |
0.000 |
18.407 |
|
| Polar |
| 3z2-r2 | 36.815 |
| x2-y2 | 13.535 |
| 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 |
2.424 |
0.000 |
0.000 |
| y |
0.000 |
2.962 |
0.000 |
| z |
0.000 |
0.000 |
6.275 |
<r2> (average value of r
2) Å
2
| <r2> |
61.792 |
| (<r2>)1/2 |
7.861 |