Vibrational Frequencies calculated at HSEh1PBE/aug-cc-pVDZ
| 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 |
1920 |
1847 |
444.47 |
|
|
|
| 2 |
A1 |
1110 |
1068 |
116.00 |
|
|
|
| 3 |
A1 |
886 |
853 |
162.84 |
|
|
|
| 4 |
A1 |
732 |
704 |
77.41 |
|
|
|
| 5 |
B1 |
792 |
762 |
31.44 |
|
|
|
| 6 |
B1 |
296 |
285 |
75.98 |
|
|
|
| 7 |
B2 |
1223 |
1177 |
451.14 |
|
|
|
| 8 |
B2 |
761 |
732 |
60.97 |
|
|
|
| 9 |
B2 |
573 |
552 |
1.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4145.8 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 3989.1 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 HSEh1PBE/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.296 |
|
|
|
| 2 |
O |
-0.416 |
|
|
|
| 3 |
Be |
0.272 |
|
|
|
| 4 |
O |
-0.576 |
|
|
|
| 5 |
O |
-0.576 |
|
|
|
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 |
-6.809 |
6.809 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.403 |
0.000 |
0.000 |
| y |
0.000 |
-31.647 |
0.000 |
| z |
0.000 |
0.000 |
-16.781 |
|
| Traceless |
| | x | y | z |
| x |
-0.188 |
0.000 |
0.000 |
| y |
0.000 |
-11.055 |
0.000 |
| z |
0.000 |
0.000 |
11.244 |
|
| Polar |
| 3z2-r2 | 22.487 |
| x2-y2 | 7.245 |
| 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 |
3.367 |
0.000 |
0.000 |
| y |
0.000 |
4.364 |
0.000 |
| z |
0.000 |
0.000 |
6.263 |
<r2> (average value of r
2) Å
2
| <r2> |
67.017 |
| (<r2>)1/2 |
8.186 |