Vibrational Frequencies calculated at LSDA/6-311G*
| 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 |
3067 |
3017 |
24.28 |
|
|
|
| 2 |
A1 |
2756 |
2711 |
13.88 |
|
|
|
| 3 |
A1 |
1503 |
1478 |
62.31 |
|
|
|
| 4 |
A1 |
1214 |
1194 |
22.77 |
|
|
|
| 5 |
B1 |
670 |
659 |
85.62 |
|
|
|
| 6 |
B1 |
602 |
593 |
31.02 |
|
|
|
| 7 |
B2 |
3133 |
3082 |
6.55 |
|
|
|
| 8 |
B2 |
882 |
868 |
42.83 |
|
|
|
| 9 |
B2 |
357 |
351 |
8.89 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7091.7 cm
-1
Scaled (by 0.9837) Zero Point Vibrational Energy (zpe) 6976.1 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 LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.815 |
|
|
|
| 2 |
B |
0.169 |
|
|
|
| 3 |
H |
0.244 |
|
|
|
| 4 |
H |
0.244 |
|
|
|
| 5 |
H |
0.158 |
|
|
|
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 |
-0.326 |
0.326 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.224 |
0.000 |
0.000 |
| y |
0.000 |
-11.638 |
0.000 |
| z |
0.000 |
0.000 |
-11.278 |
|
| Traceless |
| | x | y | z |
| x |
-4.766 |
0.000 |
0.000 |
| y |
0.000 |
2.113 |
0.000 |
| z |
0.000 |
0.000 |
2.653 |
|
| Polar |
| 3z2-r2 | 5.306 |
| x2-y2 | -4.586 |
| 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 |
2.646 |
0.000 |
0.000 |
| y |
0.000 |
2.849 |
0.000 |
| z |
0.000 |
0.000 |
5.431 |
<r2> (average value of r
2) Å
2
| <r2> |
21.639 |
| (<r2>)1/2 |
4.652 |