Vibrational Frequencies calculated at B3LYPultrafine/aug-cc-pVDZ
| 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 |
1761 |
1709 |
445.42 |
|
|
|
| 2 |
A1 |
901 |
875 |
72.46 |
|
|
|
| 3 |
A1 |
817 |
793 |
10.22 |
|
|
|
| 4 |
A1 |
526 |
510 |
87.75 |
|
|
|
| 5 |
B1 |
794 |
770 |
12.59 |
|
|
|
| 6 |
B1 |
169 |
164 |
39.30 |
|
|
|
| 7 |
B2 |
996 |
966 |
550.78 |
|
|
|
| 8 |
B2 |
666 |
646 |
0.01 |
|
|
|
| 9 |
B2 |
480 |
466 |
1.31 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3555.1 cm
-1
Scaled (by 0.9704) Zero Point Vibrational Energy (zpe) 3449.9 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 B3LYPultrafine/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.707 |
|
|
|
| 2 |
O |
-0.504 |
|
|
|
| 3 |
Mg |
1.370 |
|
|
|
| 4 |
O |
-0.787 |
|
|
|
| 5 |
O |
-0.787 |
|
|
|
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 |
11.630 |
11.630 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.939 |
0.000 |
0.000 |
| y |
0.000 |
-37.519 |
0.000 |
| z |
0.000 |
0.000 |
-17.810 |
|
| Traceless |
| | x | y | z |
| x |
-0.274 |
0.000 |
0.000 |
| y |
0.000 |
-14.644 |
0.000 |
| z |
0.000 |
0.000 |
14.918 |
|
| Polar |
| 3z2-r2 | 29.837 |
| x2-y2 | 9.580 |
| 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 |
4.423 |
0.000 |
0.000 |
| y |
0.000 |
5.535 |
0.000 |
| z |
0.000 |
0.000 |
9.994 |
<r2> (average value of r
2) Å
2
| <r2> |
98.873 |
| (<r2>)1/2 |
9.944 |