Vibrational Frequencies calculated at HSEh1PBE/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 |
2671 |
2555 |
39.27 |
|
|
|
| 2 |
A1 |
2107 |
2016 |
87.97 |
|
|
|
| 3 |
A1 |
1276 |
1221 |
30.47 |
|
|
|
| 4 |
A1 |
881 |
843 |
5.95 |
|
|
|
| 5 |
A2 |
617 |
591 |
0.00 |
|
|
|
| 6 |
B1 |
2790 |
2669 |
94.65 |
|
|
|
| 7 |
B1 |
1078 |
1031 |
0.12 |
|
|
|
| 8 |
B2 |
1980 |
1894 |
2.30 |
|
|
|
| 9 |
B2 |
759 |
726 |
0.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7080.1 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 6772.9 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 HSEh1PBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.195 |
|
|
|
| 2 |
H |
0.064 |
|
|
|
| 3 |
H |
0.064 |
|
|
|
| 4 |
H |
0.034 |
|
|
|
| 5 |
H |
0.034 |
|
|
|
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 |
-1.261 |
1.261 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.061 |
0.000 |
0.000 |
| y |
0.000 |
-9.600 |
0.000 |
| z |
0.000 |
0.000 |
-8.475 |
|
| Traceless |
| | x | y | z |
| x |
-1.023 |
0.000 |
0.000 |
| y |
0.000 |
-0.332 |
0.000 |
| z |
0.000 |
0.000 |
1.356 |
|
| Polar |
| 3z2-r2 | 2.711 |
| x2-y2 | -0.461 |
| 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 |
2.247 |
0.000 |
0.000 |
| y |
0.000 |
1.904 |
0.000 |
| z |
0.000 |
0.000 |
3.252 |
<r2> (average value of r
2) Å
2
| <r2> |
11.819 |
| (<r2>)1/2 |
3.438 |