Vibrational Frequencies calculated at HF/6-311G**
| 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 |
1977 |
1796 |
734.49 |
|
|
|
| 2 |
A1 |
1049 |
953 |
106.88 |
|
|
|
| 3 |
A1 |
911 |
828 |
38.11 |
|
|
|
| 4 |
A1 |
581 |
528 |
123.37 |
|
|
|
| 5 |
B1 |
939 |
853 |
59.97 |
|
|
|
| 6 |
B1 |
178 |
161 |
53.46 |
|
|
|
| 7 |
B2 |
1247 |
1132 |
688.67 |
|
|
|
| 8 |
B2 |
765 |
695 |
0.90 |
|
|
|
| 9 |
B2 |
542 |
493 |
10.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4094.1 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 3719.5 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.781 |
|
|
|
| 2 |
O |
-0.494 |
|
|
|
| 3 |
Mg |
1.160 |
|
|
|
| 4 |
O |
-0.724 |
|
|
|
| 5 |
O |
-0.724 |
|
|
|
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 |
13.191 |
13.191 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.449 |
0.000 |
0.000 |
| y |
0.000 |
-37.459 |
0.000 |
| z |
0.000 |
0.000 |
-15.140 |
|
| Traceless |
| | x | y | z |
| x |
-0.149 |
0.000 |
0.000 |
| y |
0.000 |
-16.665 |
0.000 |
| z |
0.000 |
0.000 |
16.814 |
|
| Polar |
| 3z2-r2 | 33.628 |
| x2-y2 | 11.011 |
| 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 |
2.556 |
0.000 |
0.000 |
| y |
0.000 |
3.116 |
0.000 |
| z |
0.000 |
0.000 |
5.756 |
<r2> (average value of r
2) Å
2
| <r2> |
95.779 |
| (<r2>)1/2 |
9.787 |