Vibrational Frequencies calculated at HSEh1PBE/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 |
1798 |
1730 |
467.72 |
|
|
|
| 2 |
A1 |
934 |
899 |
72.76 |
|
|
|
| 3 |
A1 |
828 |
797 |
12.87 |
|
|
|
| 4 |
A1 |
534 |
514 |
93.01 |
|
|
|
| 5 |
B1 |
812 |
782 |
13.20 |
|
|
|
| 6 |
B1 |
169 |
163 |
41.11 |
|
|
|
| 7 |
B2 |
1059 |
1019 |
574.70 |
|
|
|
| 8 |
B2 |
683 |
657 |
0.90 |
|
|
|
| 9 |
B2 |
490 |
471 |
2.74 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3653.6 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 3515.5 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 HSEh1PBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.805 |
|
|
|
| 2 |
O |
-0.551 |
|
|
|
| 3 |
Mg |
1.384 |
|
|
|
| 4 |
O |
-0.819 |
|
|
|
| 5 |
O |
-0.819 |
|
|
|
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 |
11.858 |
11.858 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.726 |
0.000 |
0.000 |
| y |
0.000 |
-37.205 |
0.000 |
| z |
0.000 |
0.000 |
-17.268 |
|
| Traceless |
| | x | y | z |
| x |
-0.490 |
0.000 |
0.000 |
| y |
0.000 |
-14.708 |
0.000 |
| z |
0.000 |
0.000 |
15.197 |
|
| Polar |
| 3z2-r2 | 30.395 |
| x2-y2 | 9.479 |
| 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 |
4.305 |
0.000 |
0.000 |
| y |
0.000 |
5.338 |
0.000 |
| z |
0.000 |
0.000 |
9.447 |
<r2> (average value of r
2) Å
2
| <r2> |
97.923 |
| (<r2>)1/2 |
9.896 |