Vibrational Frequencies calculated at HF/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 |
1939 |
1765 |
761.89 |
|
|
|
| 2 |
A1 |
1049 |
955 |
107.91 |
|
|
|
| 3 |
A1 |
920 |
838 |
44.36 |
|
|
|
| 4 |
A1 |
582 |
530 |
129.39 |
|
|
|
| 5 |
B1 |
938 |
854 |
45.78 |
|
|
|
| 6 |
B1 |
179 |
163 |
48.65 |
|
|
|
| 7 |
B2 |
1258 |
1145 |
671.63 |
|
|
|
| 8 |
B2 |
771 |
702 |
1.19 |
|
|
|
| 9 |
B2 |
553 |
503 |
13.83 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4093.5 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 3726.7 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.544 |
|
|
|
| 2 |
O |
-0.546 |
|
|
|
| 3 |
Mg |
1.172 |
|
|
|
| 4 |
O |
-0.585 |
|
|
|
| 5 |
O |
-0.585 |
|
|
|
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 |
13.156 |
13.156 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.744 |
0.000 |
0.000 |
| y |
0.000 |
-37.185 |
0.000 |
| z |
0.000 |
0.000 |
-16.082 |
|
| Traceless |
| | x | y | z |
| x |
-0.110 |
0.000 |
0.000 |
| y |
0.000 |
-15.772 |
0.000 |
| z |
0.000 |
0.000 |
15.882 |
|
| Polar |
| 3z2-r2 | 31.765 |
| x2-y2 | 10.441 |
| 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 |
3.528 |
0.000 |
0.000 |
| y |
0.000 |
4.242 |
0.000 |
| z |
0.000 |
0.000 |
6.189 |
<r2> (average value of r
2) Å
2
| <r2> |
94.926 |
| (<r2>)1/2 |
9.743 |