Vibrational Frequencies calculated at mPW1PW91/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 |
1923 |
1843 |
449.57 |
|
|
|
| 2 |
A1 |
1112 |
1065 |
120.00 |
|
|
|
| 3 |
A1 |
888 |
851 |
164.07 |
|
|
|
| 4 |
A1 |
734 |
703 |
76.87 |
|
|
|
| 5 |
B1 |
794 |
761 |
32.46 |
|
|
|
| 6 |
B1 |
297 |
284 |
76.88 |
|
|
|
| 7 |
B2 |
1226 |
1175 |
452.09 |
|
|
|
| 8 |
B2 |
766 |
734 |
60.72 |
|
|
|
| 9 |
B2 |
575 |
551 |
1.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4156.7 cm
-1
Scaled (by 0.9583) Zero Point Vibrational Energy (zpe) 3983.3 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 mPW1PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.306 |
|
|
|
| 2 |
O |
-0.426 |
|
|
|
| 3 |
Be |
0.260 |
|
|
|
| 4 |
O |
-0.570 |
|
|
|
| 5 |
O |
-0.570 |
|
|
|
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 |
-6.841 |
6.841 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.346 |
0.000 |
0.000 |
| y |
0.000 |
-31.617 |
0.000 |
| z |
0.000 |
0.000 |
-16.686 |
|
| Traceless |
| | x | y | z |
| x |
-0.195 |
0.000 |
0.000 |
| y |
0.000 |
-11.101 |
0.000 |
| z |
0.000 |
0.000 |
11.295 |
|
| Polar |
| 3z2-r2 | 22.590 |
| x2-y2 | 7.271 |
| 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 |
3.343 |
0.000 |
0.000 |
| y |
0.000 |
4.330 |
0.000 |
| z |
0.000 |
0.000 |
6.200 |
<r2> (average value of r
2) Å
2
| <r2> |
66.954 |
| (<r2>)1/2 |
8.183 |