Vibrational Frequencies calculated at B3LYP/CEP-31G*
| 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 |
1910 |
1845 |
437.58 |
|
|
|
| 2 |
A1 |
1094 |
1057 |
129.13 |
|
|
|
| 3 |
A1 |
852 |
823 |
151.80 |
|
|
|
| 4 |
A1 |
732 |
707 |
81.82 |
|
|
|
| 5 |
B1 |
760 |
734 |
33.36 |
|
|
|
| 6 |
B1 |
300 |
289 |
78.92 |
|
|
|
| 7 |
B2 |
1206 |
1165 |
406.33 |
|
|
|
| 8 |
B2 |
737 |
712 |
88.02 |
|
|
|
| 9 |
B2 |
555 |
536 |
2.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4073.3 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 3933.6 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 B3LYP/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.142 |
|
|
|
| 2 |
O |
-0.039 |
|
|
|
| 3 |
Be |
0.112 |
|
|
|
| 4 |
O |
-0.108 |
|
|
|
| 5 |
O |
-0.108 |
|
|
|
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 |
-6.573 |
6.573 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.103 |
0.000 |
0.000 |
| y |
0.000 |
-31.650 |
0.000 |
| z |
0.000 |
0.000 |
-16.551 |
|
| Traceless |
| | x | y | z |
| x |
-0.002 |
0.000 |
0.000 |
| y |
0.000 |
-11.323 |
0.000 |
| z |
0.000 |
0.000 |
11.326 |
|
| Polar |
| 3z2-r2 | 22.651 |
| x2-y2 | 7.547 |
| 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 |
2.699 |
0.000 |
0.000 |
| y |
0.000 |
3.577 |
0.000 |
| z |
0.000 |
0.000 |
5.920 |
<r2> (average value of r
2) Å
2
| <r2> |
52.567 |
| (<r2>)1/2 |
7.250 |