Vibrational Frequencies calculated at B3PW91/3-21G*
| 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 |
1835 |
1761 |
326.60 |
|
|
|
| 2 |
A1 |
846 |
812 |
50.27 |
|
|
|
| 3 |
A1 |
819 |
786 |
29.99 |
|
|
|
| 4 |
A1 |
533 |
512 |
68.22 |
|
|
|
| 5 |
B1 |
760 |
729 |
16.22 |
|
|
|
| 6 |
B1 |
169 |
162 |
46.35 |
|
|
|
| 7 |
B2 |
917 |
880 |
384.28 |
|
|
|
| 8 |
B2 |
660 |
633 |
17.53 |
|
|
|
| 9 |
B2 |
507 |
487 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3523.3 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3380.2 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 B3PW91/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.738 |
|
|
|
| 2 |
O |
-0.516 |
|
|
|
| 3 |
Mg |
0.827 |
|
|
|
| 4 |
O |
-0.524 |
|
|
|
| 5 |
O |
-0.524 |
|
|
|
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 |
10.358 |
10.358 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.258 |
0.000 |
0.000 |
| y |
0.000 |
-37.323 |
0.000 |
| z |
0.000 |
0.000 |
-17.099 |
|
| Traceless |
| | x | y | z |
| x |
-0.047 |
0.000 |
0.000 |
| y |
0.000 |
-15.144 |
0.000 |
| z |
0.000 |
0.000 |
15.191 |
|
| Polar |
| 3z2-r2 | 30.383 |
| x2-y2 | 10.065 |
| 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 |
3.069 |
0.000 |
0.000 |
| y |
0.000 |
3.907 |
0.000 |
| z |
0.000 |
0.000 |
8.803 |
<r2> (average value of r
2) Å
2
| <r2> |
99.740 |
| (<r2>)1/2 |
9.987 |