Vibrational Frequencies calculated at B3PW91/aug-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 |
2627 |
2534 |
36.53 |
|
|
|
| 2 |
A1 |
2152 |
2075 |
86.13 |
|
|
|
| 3 |
A1 |
1379 |
1331 |
38.15 |
|
|
|
| 4 |
A1 |
1000 |
964 |
0.08 |
|
|
|
| 5 |
A2 |
677 |
653 |
0.00 |
|
|
|
| 6 |
B1 |
2751 |
2653 |
79.29 |
|
|
|
| 7 |
B1 |
1029 |
993 |
0.50 |
|
|
|
| 8 |
B2 |
2002 |
1932 |
0.10 |
|
|
|
| 9 |
B2 |
709 |
684 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7162.7 cm
-1
Scaled (by 0.9646) Zero Point Vibrational Energy (zpe) 6909.1 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 B3PW91/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-2.136 |
|
|
|
| 2 |
H |
0.543 |
|
|
|
| 3 |
H |
0.543 |
|
|
|
| 4 |
H |
0.525 |
|
|
|
| 5 |
H |
0.525 |
|
|
|
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 |
-1.322 |
1.322 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.348 |
0.000 |
0.000 |
| y |
0.000 |
-9.943 |
0.000 |
| z |
0.000 |
0.000 |
-8.412 |
|
| Traceless |
| | x | y | z |
| x |
-1.171 |
0.000 |
0.000 |
| y |
0.000 |
-0.562 |
0.000 |
| z |
0.000 |
0.000 |
1.733 |
|
| Polar |
| 3z2-r2 | 3.467 |
| x2-y2 | -0.406 |
| 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 |
3.220 |
0.000 |
0.000 |
| y |
0.000 |
3.525 |
0.000 |
| z |
0.000 |
0.000 |
3.760 |
<r2> (average value of r
2) Å
2
| <r2> |
12.004 |
| (<r2>)1/2 |
3.465 |