Vibrational Frequencies calculated at HF/daug-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 |
2066 |
1869 |
655.27 |
|
|
|
| 2 |
A1 |
1217 |
1101 |
164.06 |
|
|
|
| 3 |
A1 |
1008 |
912 |
229.03 |
|
|
|
| 4 |
A1 |
820 |
742 |
72.77 |
|
|
|
| 5 |
B1 |
912 |
825 |
68.72 |
|
|
|
| 6 |
B1 |
325 |
294 |
87.23 |
|
|
|
| 7 |
B2 |
1350 |
1221 |
605.80 |
|
|
|
| 8 |
B2 |
911 |
824 |
26.35 |
|
|
|
| 9 |
B2 |
647 |
585 |
1.34 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4627.9 cm
-1
Scaled (by 0.9046) Zero Point Vibrational Energy (zpe) 4186.4 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/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.495 |
|
|
|
| 2 |
O |
-1.192 |
|
|
|
| 3 |
Be |
0.741 |
|
|
|
| 4 |
O |
-0.522 |
|
|
|
| 5 |
O |
-0.522 |
|
|
|
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 |
-7.556 |
7.556 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.713 |
0.000 |
0.000 |
| y |
0.000 |
-31.802 |
0.000 |
| z |
0.000 |
0.000 |
-16.154 |
|
| Traceless |
| | x | y | z |
| x |
0.264 |
0.000 |
0.000 |
| y |
0.000 |
-11.868 |
0.000 |
| z |
0.000 |
0.000 |
11.604 |
|
| Polar |
| 3z2-r2 | 23.207 |
| x2-y2 | 8.088 |
| 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 |
2.981 |
0.000 |
0.000 |
| y |
0.000 |
3.716 |
0.000 |
| z |
0.000 |
0.000 |
5.083 |
<r2> (average value of r
2) Å
2
| <r2> |
64.718 |
| (<r2>)1/2 |
8.045 |