Vibrational Frequencies calculated at PBE1PBE/STO-3G
| 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 |
1897 |
1673 |
151.47 |
|
|
|
| 2 |
A1 |
954 |
842 |
10.35 |
|
|
|
| 3 |
A1 |
913 |
806 |
49.46 |
|
|
|
| 4 |
A1 |
569 |
502 |
44.72 |
|
|
|
| 5 |
B1 |
670 |
591 |
13.78 |
|
|
|
| 6 |
B1 |
164 |
144 |
37.29 |
|
|
|
| 7 |
B2 |
1121 |
989 |
170.47 |
|
|
|
| 8 |
B2 |
804 |
709 |
0.16 |
|
|
|
| 9 |
B2 |
504 |
445 |
0.94 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3797.4 cm
-1
Scaled (by 0.8821) Zero Point Vibrational Energy (zpe) 3349.7 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 PBE1PBE/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.146 |
|
|
|
| 2 |
O |
-0.277 |
|
|
|
| 3 |
Mg |
0.890 |
|
|
|
| 4 |
O |
-0.380 |
|
|
|
| 5 |
O |
-0.380 |
|
|
|
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 |
9.245 |
9.245 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.932 |
0.000 |
0.000 |
| y |
0.000 |
-30.657 |
0.000 |
| z |
0.000 |
0.000 |
-16.517 |
|
| Traceless |
| | x | y | z |
| x |
0.655 |
0.000 |
0.000 |
| y |
0.000 |
-10.933 |
0.000 |
| z |
0.000 |
0.000 |
10.278 |
|
| Polar |
| 3z2-r2 | 20.556 |
| x2-y2 | 7.725 |
| 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 |
1.064 |
0.000 |
0.000 |
| y |
0.000 |
1.930 |
0.000 |
| z |
0.000 |
0.000 |
5.797 |
<r2> (average value of r
2) Å
2
| <r2> |
95.948 |
| (<r2>)1/2 |
9.795 |