Vibrational Frequencies calculated at B1B95/6-31G
| 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 |
2676 |
2552 |
42.17 |
|
|
|
| 2 |
A1 |
2096 |
1999 |
89.59 |
|
|
|
| 3 |
A1 |
1269 |
1210 |
27.27 |
|
|
|
| 4 |
A1 |
873 |
833 |
4.62 |
|
|
|
| 5 |
A2 |
587 |
559 |
0.00 |
|
|
|
| 6 |
B1 |
2793 |
2664 |
99.41 |
|
|
|
| 7 |
B1 |
1078 |
1028 |
0.30 |
|
|
|
| 8 |
B2 |
1954 |
1864 |
2.93 |
|
|
|
| 9 |
B2 |
774 |
738 |
0.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7050.4 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 6723.9 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 B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.175 |
|
|
|
| 2 |
H |
0.059 |
|
|
|
| 3 |
H |
0.059 |
|
|
|
| 4 |
H |
0.029 |
|
|
|
| 5 |
H |
0.029 |
|
|
|
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 |
-1.206 |
1.206 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.052 |
0.000 |
0.000 |
| y |
0.000 |
-9.468 |
0.000 |
| z |
0.000 |
0.000 |
-8.537 |
|
| Traceless |
| | x | y | z |
| x |
-1.050 |
0.000 |
0.000 |
| y |
0.000 |
-0.174 |
0.000 |
| z |
0.000 |
0.000 |
1.223 |
|
| Polar |
| 3z2-r2 | 2.447 |
| x2-y2 | -0.584 |
| 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 |
2.245 |
0.000 |
0.000 |
| y |
0.000 |
1.917 |
0.000 |
| z |
0.000 |
0.000 |
3.210 |
<r2> (average value of r
2) Å
2
| <r2> |
11.793 |
| (<r2>)1/2 |
3.434 |