Vibrational Frequencies calculated at BLYP/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 |
2585 |
2575 |
36.50 |
|
|
|
| 2 |
A1 |
2058 |
2050 |
85.15 |
|
|
|
| 3 |
A1 |
1301 |
1296 |
37.70 |
|
|
|
| 4 |
A1 |
943 |
940 |
0.75 |
|
|
|
| 5 |
A2 |
601 |
599 |
0.00 |
|
|
|
| 6 |
B1 |
2699 |
2688 |
84.57 |
|
|
|
| 7 |
B1 |
1030 |
1026 |
0.45 |
|
|
|
| 8 |
B2 |
1888 |
1881 |
0.27 |
|
|
|
| 9 |
B2 |
724 |
721 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6914.1 cm
-1
Scaled (by 0.9961) Zero Point Vibrational Energy (zpe) 6887.2 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 BLYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.170 |
|
|
|
| 2 |
H |
0.081 |
|
|
|
| 3 |
H |
0.081 |
|
|
|
| 4 |
H |
0.004 |
|
|
|
| 5 |
H |
0.004 |
|
|
|
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 |
-1.285 |
1.285 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.455 |
0.000 |
0.000 |
| y |
0.000 |
-9.908 |
0.000 |
| z |
0.000 |
0.000 |
-8.644 |
|
| Traceless |
| | x | y | z |
| x |
-1.178 |
0.000 |
0.000 |
| y |
0.000 |
-0.358 |
0.000 |
| z |
0.000 |
0.000 |
1.537 |
|
| Polar |
| 3z2-r2 | 3.073 |
| x2-y2 | -0.547 |
| 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 |
2.739 |
0.000 |
0.000 |
| y |
0.000 |
2.432 |
0.000 |
| z |
0.000 |
0.000 |
3.646 |
<r2> (average value of r
2) Å
2
| <r2> |
12.021 |
| (<r2>)1/2 |
3.467 |