Vibrational Frequencies calculated at PBEPBE/6-311G**
| 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 |
1746 |
1730 |
559.68 |
|
|
|
| 2 |
A1 |
915 |
907 |
72.36 |
|
|
|
| 3 |
A1 |
740 |
733 |
66.30 |
|
|
|
| 4 |
A1 |
445 |
441 |
61.21 |
|
|
|
| 5 |
B1 |
784 |
777 |
14.20 |
|
|
|
| 6 |
B1 |
111 |
110 |
18.12 |
|
|
|
| 7 |
B2 |
1019 |
1010 |
302.36 |
|
|
|
| 8 |
B2 |
631 |
625 |
0.83 |
|
|
|
| 9 |
B2 |
362 |
359 |
8.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3376.2 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 3345.5 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 PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.409 |
|
|
|
| 2 |
O |
-0.351 |
|
|
|
| 3 |
Ca |
1.014 |
|
|
|
| 4 |
O |
-0.536 |
|
|
|
| 5 |
O |
-0.536 |
|
|
|
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 |
12.250 |
12.250 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.620 |
0.000 |
0.000 |
| y |
0.000 |
-41.644 |
0.000 |
| z |
0.000 |
0.000 |
-29.247 |
|
| Traceless |
| | x | y | z |
| x |
3.826 |
0.000 |
0.000 |
| y |
0.000 |
-11.210 |
0.000 |
| z |
0.000 |
0.000 |
7.385 |
|
| Polar |
| 3z2-r2 | 14.769 |
| x2-y2 | 10.024 |
| 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 |
3.050 |
0.000 |
0.000 |
| y |
0.000 |
5.475 |
0.000 |
| z |
0.000 |
0.000 |
10.208 |
<r2> (average value of r
2) Å
2
| <r2> |
132.425 |
| (<r2>)1/2 |
11.508 |