Vibrational Frequencies calculated at HSEh1PBE/6-311G**
| 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 |
3155 |
3030 |
14.15 |
|
|
|
| 2 |
A1 |
2831 |
2719 |
17.78 |
|
|
|
| 3 |
A1 |
1519 |
1459 |
57.39 |
|
|
|
| 4 |
A1 |
1267 |
1217 |
10.63 |
|
|
|
| 5 |
B1 |
728 |
699 |
90.98 |
|
|
|
| 6 |
B1 |
651 |
625 |
6.04 |
|
|
|
| 7 |
B2 |
3226 |
3098 |
2.43 |
|
|
|
| 8 |
B2 |
913 |
877 |
47.65 |
|
|
|
| 9 |
B2 |
403 |
387 |
3.48 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7346.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 7055.8 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.546 |
|
|
|
| 2 |
B |
0.208 |
|
|
|
| 3 |
H |
0.138 |
|
|
|
| 4 |
H |
0.138 |
|
|
|
| 5 |
H |
0.064 |
|
|
|
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 |
-0.515 |
0.515 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.998 |
0.000 |
0.000 |
| y |
0.000 |
-11.540 |
0.000 |
| z |
0.000 |
0.000 |
-11.381 |
|
| Traceless |
| | x | y | z |
| x |
-4.537 |
0.000 |
0.000 |
| y |
0.000 |
2.149 |
0.000 |
| z |
0.000 |
0.000 |
2.388 |
|
| Polar |
| 3z2-r2 | 4.775 |
| x2-y2 | -4.457 |
| 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 |
2.669 |
0.000 |
0.000 |
| y |
0.000 |
2.775 |
0.000 |
| z |
0.000 |
0.000 |
5.426 |
<r2> (average value of r
2) Å
2
| <r2> |
21.544 |
| (<r2>)1/2 |
4.642 |