Vibrational Frequencies calculated at HF/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 |
1943 |
1765 |
908.15 |
|
|
|
| 2 |
A1 |
1084 |
984 |
109.61 |
|
|
|
| 3 |
A1 |
840 |
763 |
84.91 |
|
|
|
| 4 |
A1 |
482 |
438 |
133.15 |
|
|
|
| 5 |
B1 |
955 |
868 |
62.58 |
|
|
|
| 6 |
B1 |
130 |
118 |
26.92 |
|
|
|
| 7 |
B2 |
1303 |
1184 |
577.77 |
|
|
|
| 8 |
B2 |
749 |
681 |
1.14 |
|
|
|
| 9 |
B2 |
411 |
373 |
20.79 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3948.7 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 3587.3 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 HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.718 |
|
|
|
| 2 |
O |
-0.531 |
|
|
|
| 3 |
Ca |
1.399 |
|
|
|
| 4 |
O |
-0.793 |
|
|
|
| 5 |
O |
-0.793 |
|
|
|
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 |
15.731 |
15.731 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-30.968 |
0.000 |
0.000 |
| y |
0.000 |
-42.641 |
0.000 |
| z |
0.000 |
0.000 |
-27.086 |
|
| Traceless |
| | x | y | z |
| x |
3.895 |
0.000 |
0.000 |
| y |
0.000 |
-13.614 |
0.000 |
| z |
0.000 |
0.000 |
9.719 |
|
| Polar |
| 3z2-r2 | 19.438 |
| x2-y2 | 11.673 |
| 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 |
2.467 |
0.000 |
0.000 |
| y |
0.000 |
3.575 |
0.000 |
| z |
0.000 |
0.000 |
6.204 |
<r2> (average value of r
2) Å
2
| <r2> |
131.696 |
| (<r2>)1/2 |
11.476 |