Vibrational Frequencies calculated at PBEPBEultrafine/aug-cc-pVTZ
| 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 |
1709 |
1690 |
353.35 |
|
|
|
| 2 |
A1 |
865 |
855 |
58.56 |
|
|
|
| 3 |
A1 |
787 |
778 |
4.19 |
|
|
|
| 4 |
A1 |
505 |
499 |
71.45 |
|
|
|
| 5 |
B1 |
761 |
753 |
5.60 |
|
|
|
| 6 |
B1 |
159 |
157 |
35.49 |
|
|
|
| 7 |
B2 |
898 |
888 |
540.86 |
|
|
|
| 8 |
B2 |
634 |
627 |
1.23 |
|
|
|
| 9 |
B2 |
434 |
429 |
3.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3376.1 cm
-1
Scaled (by 0.9888) Zero Point Vibrational Energy (zpe) 3338.3 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 PBEPBEultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.539 |
|
|
|
| 2 |
O |
-0.427 |
|
|
|
| 3 |
Mg |
0.830 |
|
|
|
| 4 |
O |
-0.471 |
|
|
|
| 5 |
O |
-0.471 |
|
|
|
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 |
10.956 |
10.956 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-28.040 |
0.000 |
0.000 |
| y |
0.000 |
-37.271 |
0.000 |
| z |
0.000 |
0.000 |
-18.550 |
|
| Traceless |
| | x | y | z |
| x |
-0.129 |
0.000 |
0.000 |
| y |
0.000 |
-13.976 |
0.000 |
| z |
0.000 |
0.000 |
14.105 |
|
| Polar |
| 3z2-r2 | 28.211 |
| x2-y2 | 9.231 |
| 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 |
4.912 |
0.000 |
0.000 |
| y |
0.000 |
6.359 |
0.000 |
| z |
0.000 |
0.000 |
11.409 |
<r2> (average value of r
2) Å
2
| <r2> |
99.402 |
| (<r2>)1/2 |
9.970 |