Vibrational Frequencies calculated at PBE1PBE/TZVP
| 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 |
1947 |
1868 |
448.49 |
|
|
|
| 2 |
A1 |
1113 |
1068 |
116.79 |
|
|
|
| 3 |
A1 |
893 |
857 |
173.14 |
|
|
|
| 4 |
A1 |
761 |
730 |
76.52 |
|
|
|
| 5 |
B1 |
808 |
775 |
35.28 |
|
|
|
| 6 |
B1 |
302 |
290 |
75.93 |
|
|
|
| 7 |
B2 |
1218 |
1169 |
490.81 |
|
|
|
| 8 |
B2 |
753 |
723 |
49.39 |
|
|
|
| 9 |
B2 |
584 |
561 |
3.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4189.7 cm
-1
Scaled (by 0.9596) Zero Point Vibrational Energy (zpe) 4020.5 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 PBE1PBE/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.228 |
|
|
|
| 2 |
O |
-0.271 |
|
|
|
| 3 |
Be |
0.608 |
|
|
|
| 4 |
O |
-0.283 |
|
|
|
| 5 |
O |
-0.283 |
|
|
|
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 |
-6.754 |
6.754 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.150 |
0.000 |
0.000 |
| y |
0.000 |
-31.945 |
0.000 |
| z |
0.000 |
0.000 |
-16.922 |
|
| Traceless |
| | x | y | z |
| x |
0.284 |
0.000 |
0.000 |
| y |
0.000 |
-11.409 |
0.000 |
| z |
0.000 |
0.000 |
11.125 |
|
| Polar |
| 3z2-r2 | 22.249 |
| x2-y2 | 7.795 |
| 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 |
2.670 |
0.000 |
0.000 |
| y |
0.000 |
3.698 |
0.000 |
| z |
0.000 |
0.000 |
5.885 |
<r2> (average value of r
2) Å
2
| <r2> |
66.746 |
| (<r2>)1/2 |
8.170 |