Vibrational Frequencies calculated at wB97X-D/6-31+G**
| 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 |
3174 |
3023 |
8.87 |
|
|
|
| 2 |
A1 |
2838 |
2703 |
29.17 |
|
|
|
| 3 |
A1 |
1528 |
1455 |
64.76 |
|
|
|
| 4 |
A1 |
1282 |
1220 |
5.20 |
|
|
|
| 5 |
B1 |
754 |
718 |
118.54 |
|
|
|
| 6 |
B1 |
651 |
620 |
0.17 |
|
|
|
| 7 |
B2 |
3250 |
3095 |
1.17 |
|
|
|
| 8 |
B2 |
906 |
862 |
57.41 |
|
|
|
| 9 |
B2 |
423 |
403 |
3.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7402.7 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 7049.6 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 wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.608 |
|
|
|
| 2 |
B |
0.203 |
|
|
|
| 3 |
H |
0.178 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
| 5 |
H |
0.050 |
|
|
|
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 |
-0.670 |
0.670 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.472 |
0.000 |
0.000 |
| y |
0.000 |
-11.638 |
0.000 |
| z |
0.000 |
0.000 |
-11.492 |
|
| Traceless |
| | x | y | z |
| x |
-4.907 |
0.000 |
0.000 |
| y |
0.000 |
2.344 |
0.000 |
| z |
0.000 |
0.000 |
2.563 |
|
| Polar |
| 3z2-r2 | 5.127 |
| x2-y2 | -4.834 |
| 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 |
3.407 |
0.000 |
0.000 |
| y |
0.000 |
2.714 |
0.000 |
| z |
0.000 |
0.000 |
5.808 |
<r2> (average value of r
2) Å
2
| <r2> |
21.797 |
| (<r2>)1/2 |
4.669 |