Vibrational Frequencies calculated at LSDA/cc-pVTZ
| 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 |
2593 |
2564 |
20.42 |
|
|
|
| 2 |
A1 |
2132 |
2109 |
53.09 |
|
|
|
| 3 |
A1 |
1403 |
1388 |
30.21 |
|
|
|
| 4 |
A1 |
1001 |
990 |
0.29 |
|
|
|
| 5 |
A2 |
469 |
464 |
0.00 |
|
|
|
| 6 |
B1 |
2714 |
2684 |
48.63 |
|
|
|
| 7 |
B1 |
996 |
985 |
0.06 |
|
|
|
| 8 |
B2 |
2016 |
1994 |
1.34 |
|
|
|
| 9 |
B2 |
668 |
661 |
0.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6995.2 cm
-1
Scaled (by 0.9891) Zero Point Vibrational Energy (zpe) 6919.0 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 LSDA/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.484 |
|
|
|
| 2 |
H |
0.146 |
|
|
|
| 3 |
H |
0.146 |
|
|
|
| 4 |
H |
0.096 |
|
|
|
| 5 |
H |
0.096 |
|
|
|
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 |
-1.386 |
1.386 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.429 |
0.000 |
0.000 |
| y |
0.000 |
-10.086 |
0.000 |
| z |
0.000 |
0.000 |
-8.477 |
|
| Traceless |
| | x | y | z |
| x |
-1.147 |
0.000 |
0.000 |
| y |
0.000 |
-0.633 |
0.000 |
| z |
0.000 |
0.000 |
1.780 |
|
| Polar |
| 3z2-r2 | 3.560 |
| x2-y2 | -0.343 |
| 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 |
3.028 |
0.000 |
0.000 |
| y |
0.000 |
2.883 |
0.000 |
| z |
0.000 |
0.000 |
3.728 |
<r2> (average value of r
2) Å
2
| <r2> |
12.001 |
| (<r2>)1/2 |
3.464 |