Vibrational Frequencies calculated at BLYP/STO-3G
| 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 |
3270 |
3026 |
49.43 |
|
|
|
| 2 |
A1 |
3089 |
2858 |
7.53 |
|
|
|
| 3 |
A1 |
1625 |
1503 |
44.29 |
|
|
|
| 4 |
A1 |
1397 |
1292 |
2.00 |
|
|
|
| 5 |
B1 |
802 |
742 |
32.81 |
|
|
|
| 6 |
B1 |
661 |
612 |
9.22 |
|
|
|
| 7 |
B2 |
3374 |
3121 |
10.29 |
|
|
|
| 8 |
B2 |
966 |
894 |
79.23 |
|
|
|
| 9 |
B2 |
491 |
454 |
1.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7836.8 cm
-1
Scaled (by 0.9252) Zero Point Vibrational Energy (zpe) 7250.6 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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.330 |
|
|
|
| 2 |
B |
0.185 |
|
|
|
| 3 |
H |
0.084 |
|
|
|
| 4 |
H |
0.084 |
|
|
|
| 5 |
H |
-0.023 |
|
|
|
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 |
-0.206 |
0.206 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.115 |
0.000 |
0.000 |
| y |
0.000 |
-10.439 |
0.000 |
| z |
0.000 |
0.000 |
-11.147 |
|
| Traceless |
| | x | y | z |
| x |
-2.322 |
0.000 |
0.000 |
| y |
0.000 |
1.692 |
0.000 |
| z |
0.000 |
0.000 |
0.630 |
|
| Polar |
| 3z2-r2 | 1.261 |
| x2-y2 | -2.676 |
| 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 |
0.493 |
0.000 |
0.000 |
| y |
0.000 |
1.442 |
0.000 |
| z |
0.000 |
0.000 |
3.026 |
<r2> (average value of r
2) Å
2
| <r2> |
20.718 |
| (<r2>)1/2 |
4.552 |