Vibrational Frequencies calculated at B1B95/6-31G*
| 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 |
3187 |
3025 |
10.50 |
|
|
|
| 2 |
A1 |
2863 |
2718 |
26.48 |
|
|
|
| 3 |
A1 |
1540 |
1462 |
52.36 |
|
|
|
| 4 |
A1 |
1292 |
1226 |
5.15 |
|
|
|
| 5 |
B1 |
731 |
694 |
75.90 |
|
|
|
| 6 |
B1 |
632 |
600 |
15.08 |
|
|
|
| 7 |
B2 |
3255 |
3090 |
0.76 |
|
|
|
| 8 |
B2 |
917 |
870 |
51.30 |
|
|
|
| 9 |
B2 |
405 |
385 |
4.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7410.0 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 7034.3 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 B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.538 |
|
|
|
| 2 |
B |
0.120 |
|
|
|
| 3 |
H |
0.184 |
|
|
|
| 4 |
H |
0.184 |
|
|
|
| 5 |
H |
0.052 |
|
|
|
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 |
-0.447 |
0.447 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.318 |
0.000 |
0.000 |
| y |
0.000 |
-11.208 |
0.000 |
| z |
0.000 |
0.000 |
-11.096 |
|
| Traceless |
| | x | y | z |
| x |
-4.166 |
0.000 |
0.000 |
| y |
0.000 |
1.999 |
0.000 |
| z |
0.000 |
0.000 |
2.167 |
|
| Polar |
| 3z2-r2 | 4.334 |
| x2-y2 | -4.110 |
| 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 |
1.871 |
0.000 |
0.000 |
| y |
0.000 |
2.543 |
0.000 |
| z |
0.000 |
0.000 |
5.012 |
<r2> (average value of r
2) Å
2
| <r2> |
21.330 |
| (<r2>)1/2 |
4.618 |