Vibrational Frequencies calculated at B2PLYP/3-21G
| 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 |
2701 |
2701 |
28.44 |
|
|
|
| 2 |
A1 |
2091 |
2091 |
81.33 |
|
|
|
| 3 |
A1 |
1264 |
1264 |
37.84 |
|
|
|
| 4 |
A1 |
724 |
724 |
22.10 |
|
|
|
| 5 |
A2 |
744 |
744 |
0.00 |
|
|
|
| 6 |
B1 |
2822 |
2822 |
72.32 |
|
|
|
| 7 |
B1 |
1093 |
1093 |
0.60 |
|
|
|
| 8 |
B2 |
1956 |
1956 |
8.35 |
|
|
|
| 9 |
B2 |
785 |
785 |
0.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7089.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7089.9 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 B2PLYP/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
B |
-0.259 |
|
|
|
| 2 |
H |
0.075 |
|
|
|
| 3 |
H |
0.075 |
|
|
|
| 4 |
H |
0.054 |
|
|
|
| 5 |
H |
0.054 |
|
|
|
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 |
-1.211 |
1.211 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.428 |
0.000 |
0.000 |
| y |
0.000 |
-9.856 |
0.000 |
| z |
0.000 |
0.000 |
-8.760 |
|
| Traceless |
| | x | y | z |
| x |
-1.120 |
0.000 |
0.000 |
| y |
0.000 |
-0.262 |
0.000 |
| z |
0.000 |
0.000 |
1.382 |
|
| Polar |
| 3z2-r2 | 2.764 |
| x2-y2 | -0.572 |
| 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 |
2.078 |
0.000 |
0.000 |
| y |
0.000 |
1.850 |
0.000 |
| z |
0.000 |
0.000 |
3.079 |
<r2> (average value of r
2) Å
2
| <r2> |
11.995 |
| (<r2>)1/2 |
3.463 |