Vibrational Frequencies calculated at wB97X-D/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 |
3175 |
3175 |
3.39 |
|
|
|
| 2 |
A1 |
2817 |
2817 |
34.13 |
|
|
|
| 3 |
A1 |
1517 |
1517 |
73.30 |
|
|
|
| 4 |
A1 |
1276 |
1276 |
3.87 |
|
|
|
| 5 |
B1 |
742 |
742 |
121.72 |
|
|
|
| 6 |
B1 |
636 |
636 |
9.66 |
|
|
|
| 7 |
B2 |
3258 |
3258 |
1.26 |
|
|
|
| 8 |
B2 |
915 |
915 |
45.44 |
|
|
|
| 9 |
B2 |
400 |
400 |
6.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7367.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7367.6 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/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.151 |
|
|
|
| 2 |
B |
-0.457 |
|
|
|
| 3 |
H |
0.211 |
|
|
|
| 4 |
H |
0.211 |
|
|
|
| 5 |
H |
0.186 |
|
|
|
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 |
-0.616 |
0.616 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.116 |
0.000 |
0.000 |
| y |
0.000 |
-11.210 |
0.000 |
| z |
0.000 |
0.000 |
-10.619 |
|
| Traceless |
| | x | y | z |
| x |
-5.201 |
0.000 |
0.000 |
| y |
0.000 |
2.158 |
0.000 |
| z |
0.000 |
0.000 |
3.044 |
|
| Polar |
| 3z2-r2 | 6.088 |
| x2-y2 | -4.906 |
| 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 |
2.806 |
0.000 |
0.000 |
| y |
0.000 |
2.478 |
0.000 |
| z |
0.000 |
0.000 |
5.242 |
<r2> (average value of r
2) Å
2
| <r2> |
19.780 |
| (<r2>)1/2 |
4.448 |