Vibrational Frequencies calculated at wB97X-D/6-31G(2df,p)
| 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 |
3173 |
3173 |
10.26 |
|
|
|
| 2 |
A1 |
2836 |
2836 |
18.07 |
|
|
|
| 3 |
A1 |
1527 |
1527 |
51.44 |
|
|
|
| 4 |
A1 |
1281 |
1281 |
6.40 |
|
|
|
| 5 |
B1 |
752 |
752 |
70.60 |
|
|
|
| 6 |
B1 |
656 |
656 |
2.77 |
|
|
|
| 7 |
B2 |
3245 |
3245 |
1.05 |
|
|
|
| 8 |
B2 |
903 |
903 |
45.32 |
|
|
|
| 9 |
B2 |
393 |
393 |
1.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7382.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7382.4 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.390 |
|
|
|
| 2 |
B |
0.016 |
|
|
|
| 3 |
H |
0.158 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
| 5 |
H |
0.058 |
|
|
|
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 |
-0.501 |
0.501 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.279 |
0.000 |
0.000 |
| y |
0.000 |
-11.271 |
0.000 |
| z |
0.000 |
0.000 |
-11.126 |
|
| Traceless |
| | x | y | z |
| x |
-4.080 |
0.000 |
0.000 |
| y |
0.000 |
1.931 |
0.000 |
| z |
0.000 |
0.000 |
2.149 |
|
| Polar |
| 3z2-r2 | 4.298 |
| x2-y2 | -4.008 |
| 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 |
2.332 |
0.000 |
0.000 |
| y |
0.000 |
2.794 |
0.000 |
| z |
0.000 |
0.000 |
5.146 |
<r2> (average value of r
2) Å
2
| <r2> |
21.314 |
| (<r2>)1/2 |
4.617 |