Vibrational Frequencies calculated at B1B95/6-311G**
| 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 |
2644 |
2539 |
36.95 |
|
|
|
| 2 |
A1 |
2133 |
2048 |
87.81 |
|
|
|
| 3 |
A1 |
1354 |
1300 |
43.90 |
|
|
|
| 4 |
A1 |
987 |
948 |
0.67 |
|
|
|
| 5 |
A2 |
698 |
670 |
0.00 |
|
|
|
| 6 |
B1 |
2763 |
2653 |
85.87 |
|
|
|
| 7 |
B1 |
1045 |
1003 |
0.45 |
|
|
|
| 8 |
B2 |
2024 |
1943 |
0.63 |
|
|
|
| 9 |
B2 |
726 |
697 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7187.5 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 6900.7 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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.234 |
|
|
|
| 2 |
H |
0.097 |
|
|
|
| 3 |
H |
0.097 |
|
|
|
| 4 |
H |
0.020 |
|
|
|
| 5 |
H |
0.020 |
|
|
|
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 |
-1.307 |
1.307 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.283 |
0.000 |
0.000 |
| y |
0.000 |
-9.847 |
0.000 |
| z |
0.000 |
0.000 |
-8.431 |
|
| Traceless |
| | x | y | z |
| x |
-1.144 |
0.000 |
0.000 |
| y |
0.000 |
-0.490 |
0.000 |
| z |
0.000 |
0.000 |
1.634 |
|
| Polar |
| 3z2-r2 | 3.269 |
| x2-y2 | -0.436 |
| 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 |
2.666 |
0.000 |
0.000 |
| y |
0.000 |
2.380 |
0.000 |
| z |
0.000 |
0.000 |
3.564 |
<r2> (average value of r
2) Å
2
| <r2> |
11.858 |
| (<r2>)1/2 |
3.444 |