Vibrational Frequencies calculated at PBEPBE/6-31+G**
| 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 |
1667 |
1648 |
469.31 |
|
|
|
| 2 |
A1 |
905 |
895 |
67.03 |
|
|
|
| 3 |
A1 |
709 |
701 |
4.01 |
|
|
|
| 4 |
A1 |
415 |
410 |
67.70 |
|
|
|
| 5 |
B1 |
768 |
759 |
4.69 |
|
|
|
| 6 |
B1 |
99 |
98 |
22.96 |
|
|
|
| 7 |
B2 |
796 |
787 |
254.11 |
|
|
|
| 8 |
B2 |
464 |
459 |
60.57 |
|
|
|
| 9 |
B2 |
423i |
418i |
102.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2700.0 cm
-1
Scaled (by 0.9886) Zero Point Vibrational Energy (zpe) 2669.2 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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.516 |
|
|
|
| 2 |
O |
-0.525 |
|
|
|
| 3 |
Ca |
1.299 |
|
|
|
| 4 |
O |
-0.645 |
|
|
|
| 5 |
O |
-0.645 |
|
|
|
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 |
15.175 |
15.175 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.617 |
0.000 |
0.000 |
| y |
0.000 |
-44.854 |
0.000 |
| z |
0.000 |
0.000 |
-28.436 |
|
| Traceless |
| | x | y | z |
| x |
3.028 |
0.000 |
0.000 |
| y |
0.000 |
-13.828 |
0.000 |
| z |
0.000 |
0.000 |
10.799 |
|
| Polar |
| 3z2-r2 | 21.599 |
| x2-y2 | 11.237 |
| 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 |
5.288 |
0.000 |
0.000 |
| y |
0.000 |
7.768 |
0.000 |
| z |
0.000 |
0.000 |
15.573 |
<r2> (average value of r
2) Å
2
| <r2> |
141.082 |
| (<r2>)1/2 |
11.878 |