Vibrational Frequencies calculated at B3PW91/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 |
1866 |
1651 |
143.58 |
|
|
|
| 2 |
A1 |
940 |
832 |
10.73 |
|
|
|
| 3 |
A1 |
892 |
790 |
45.34 |
|
|
|
| 4 |
A1 |
560 |
496 |
43.42 |
|
|
|
| 5 |
B1 |
656 |
580 |
11.92 |
|
|
|
| 6 |
B1 |
162 |
143 |
36.38 |
|
|
|
| 7 |
B2 |
1090 |
965 |
163.00 |
|
|
|
| 8 |
B2 |
786 |
695 |
0.78 |
|
|
|
| 9 |
B2 |
496 |
439 |
0.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3724.2 cm
-1
Scaled (by 0.885) Zero Point Vibrational Energy (zpe) 3295.9 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 B3PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.140 |
|
|
|
| 2 |
O |
-0.274 |
|
|
|
| 3 |
Mg |
0.880 |
|
|
|
| 4 |
O |
-0.373 |
|
|
|
| 5 |
O |
-0.373 |
|
|
|
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 |
9.138 |
9.138 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.974 |
0.000 |
0.000 |
| y |
0.000 |
-30.611 |
0.000 |
| z |
0.000 |
0.000 |
-16.612 |
|
| Traceless |
| | x | y | z |
| x |
0.638 |
0.000 |
0.000 |
| y |
0.000 |
-10.818 |
0.000 |
| z |
0.000 |
0.000 |
10.180 |
|
| Polar |
| 3z2-r2 | 20.360 |
| x2-y2 | 7.638 |
| 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 |
1.100 |
0.000 |
0.000 |
| y |
0.000 |
1.983 |
0.000 |
| z |
0.000 |
0.000 |
5.964 |
<r2> (average value of r
2) Å
2
| <r2> |
96.548 |
| (<r2>)1/2 |
9.826 |