Vibrational Frequencies calculated at BLYP/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
1532 |
1520 |
182.22 |
|
|
|
| 2 |
A' |
1025 |
1017 |
560.22 |
|
|
|
| 3 |
A' |
857 |
850 |
89.14 |
|
|
|
| 4 |
A' |
695 |
689 |
14.98 |
|
|
|
| 5 |
A' |
592 |
587 |
219.27 |
|
|
|
| 6 |
A' |
389 |
386 |
2.00 |
|
|
|
| 7 |
A' |
363 |
361 |
44.19 |
|
|
|
| 8 |
A" |
753 |
747 |
4.82 |
|
|
|
| 9 |
A" |
99 |
98 |
16.28 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3152.9 cm
-1
Scaled (by 0.9919) Zero Point Vibrational Energy (zpe) 3127.3 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 BLYP/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.699 |
|
|
|
| 2 |
O |
-0.467 |
|
|
|
| 3 |
Ca |
1.002 |
|
|
|
| 4 |
O |
-0.639 |
|
|
|
| 5 |
O |
-0.595 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.679 |
-12.096 |
0.000 |
12.115 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-43.439 |
-0.756 |
0.000 |
| y |
-0.756 |
-31.378 |
0.000 |
| z |
0.000 |
0.000 |
-33.502 |
|
| Traceless |
| | x | y | z |
| x |
-10.999 |
-0.756 |
0.000 |
| y |
-0.756 |
7.093 |
0.000 |
| z |
0.000 |
0.000 |
3.906 |
|
| Polar |
| 3z2-r2 | 7.812 |
| x2-y2 | -12.061 |
| xy | -0.756 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
8.016 |
-1.062 |
0.000 |
| y |
-1.062 |
27.369 |
-0.001 |
| z |
0.000 |
-0.001 |
6.007 |
<r2> (average value of r
2) Å
2
| <r2> |
142.068 |
| (<r2>)1/2 |
11.919 |