Vibrational Frequencies calculated at HF/SDD
| 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 |
2725 |
2454 |
83.73 |
|
|
|
| 2 |
A1 |
2086 |
1879 |
216.40 |
|
|
|
| 3 |
A1 |
1269 |
1142 |
33.31 |
|
|
|
| 4 |
A1 |
683 |
615 |
25.57 |
|
|
|
| 5 |
A2 |
838 |
755 |
0.00 |
|
|
|
| 6 |
B1 |
2850 |
2566 |
171.26 |
|
|
|
| 7 |
B1 |
1100 |
991 |
1.86 |
|
|
|
| 8 |
B2 |
1811 |
1630 |
3.78 |
|
|
|
| 9 |
B2 |
797 |
718 |
1.87 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7079.5 cm
-1
Scaled (by 0.9004) Zero Point Vibrational Energy (zpe) 6374.4 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 HF/SDD
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.301 |
|
|
|
| 2 |
H |
0.083 |
|
|
|
| 3 |
H |
0.083 |
|
|
|
| 4 |
H |
0.067 |
|
|
|
| 5 |
H |
0.067 |
|
|
|
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 |
-1.253 |
1.253 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.354 |
0.000 |
0.000 |
| y |
0.000 |
-9.716 |
0.000 |
| z |
0.000 |
0.000 |
-8.844 |
|
| Traceless |
| | x | y | z |
| x |
-1.074 |
0.000 |
0.000 |
| y |
0.000 |
-0.117 |
0.000 |
| z |
0.000 |
0.000 |
1.191 |
|
| Polar |
| 3z2-r2 | 2.383 |
| x2-y2 | -0.638 |
| 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 |
1.846 |
0.000 |
0.000 |
| y |
0.000 |
2.100 |
0.000 |
| z |
0.000 |
0.000 |
2.778 |
<r2> (average value of r
2) Å
2
| <r2> |
12.015 |
| (<r2>)1/2 |
3.466 |