Vibrational Frequencies calculated at HSEh1PBE/cc-pVDZ
| 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 |
2639 |
2538 |
38.03 |
|
|
|
| 2 |
A1 |
2178 |
2095 |
85.97 |
|
|
|
| 3 |
A1 |
1371 |
1319 |
37.82 |
|
|
|
| 4 |
A1 |
994 |
956 |
0.04 |
|
|
|
| 5 |
A2 |
676 |
650 |
0.00 |
|
|
|
| 6 |
B1 |
2763 |
2657 |
82.25 |
|
|
|
| 7 |
B1 |
1022 |
983 |
0.05 |
|
|
|
| 8 |
B2 |
2016 |
1939 |
0.77 |
|
|
|
| 9 |
B2 |
716 |
689 |
0.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7187.3 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 6913.5 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.259 |
|
|
|
| 2 |
H |
0.105 |
|
|
|
| 3 |
H |
0.105 |
|
|
|
| 4 |
H |
0.025 |
|
|
|
| 5 |
H |
0.025 |
|
|
|
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 |
-1.331 |
1.331 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.152 |
0.000 |
0.000 |
| y |
0.000 |
-9.824 |
0.000 |
| z |
0.000 |
0.000 |
-8.238 |
|
| Traceless |
| | x | y | z |
| x |
-1.121 |
0.000 |
0.000 |
| y |
0.000 |
-0.630 |
0.000 |
| z |
0.000 |
0.000 |
1.750 |
|
| Polar |
| 3z2-r2 | 3.501 |
| x2-y2 | -0.328 |
| 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 |
2.629 |
0.000 |
0.000 |
| y |
0.000 |
2.284 |
0.000 |
| z |
0.000 |
0.000 |
3.512 |
<r2> (average value of r
2) Å
2
| <r2> |
11.932 |
| (<r2>)1/2 |
3.454 |