Vibrational Frequencies calculated at B3PW91/6-31G**
| 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 |
3169 |
3037 |
10.60 |
|
|
|
| 2 |
A1 |
2843 |
2725 |
22.56 |
|
|
|
| 3 |
A1 |
1525 |
1462 |
50.50 |
|
|
|
| 4 |
A1 |
1277 |
1224 |
6.09 |
|
|
|
| 5 |
B1 |
725 |
695 |
76.43 |
|
|
|
| 6 |
B1 |
625 |
599 |
10.77 |
|
|
|
| 7 |
B2 |
3241 |
3106 |
1.01 |
|
|
|
| 8 |
B2 |
916 |
878 |
49.23 |
|
|
|
| 9 |
B2 |
410 |
393 |
4.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7365.4 cm
-1
Scaled (by 0.9584) Zero Point Vibrational Energy (zpe) 7059.0 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 B3PW91/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.470 |
|
|
|
| 2 |
B |
0.152 |
|
|
|
| 3 |
H |
0.147 |
|
|
|
| 4 |
H |
0.147 |
|
|
|
| 5 |
H |
0.024 |
|
|
|
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 |
-0.429 |
0.429 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.315 |
0.000 |
0.000 |
| y |
0.000 |
-11.214 |
0.000 |
| z |
0.000 |
0.000 |
-11.093 |
|
| Traceless |
| | x | y | z |
| x |
-4.162 |
0.000 |
0.000 |
| y |
0.000 |
1.990 |
0.000 |
| z |
0.000 |
0.000 |
2.171 |
|
| Polar |
| 3z2-r2 | 4.342 |
| x2-y2 | -4.101 |
| 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 |
1.918 |
0.000 |
0.000 |
| y |
0.000 |
2.593 |
0.000 |
| z |
0.000 |
0.000 |
5.084 |
<r2> (average value of r
2) Å
2
| <r2> |
21.369 |
| (<r2>)1/2 |
4.623 |