Vibrational Frequencies calculated at B3PW91/6-311+G(3df,2p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
3514 |
3364 |
0.00 |
51.45 |
0.27 |
0.43 |
| 2 |
Σg |
2068 |
1980 |
0.00 |
107.23 |
0.07 |
0.13 |
| 3 |
Σu |
3412 |
3266 |
90.01 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
663 |
635 |
0.00 |
3.55 |
0.75 |
0.86 |
| 4 |
Πg |
663 |
635 |
0.00 |
3.55 |
0.75 |
0.86 |
| 5 |
Πu |
767 |
735 |
100.30 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
767 |
735 |
100.30 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 5927.0 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 5673.9 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 B3PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.216 |
|
|
|
| 2 |
C |
-0.216 |
|
|
|
| 3 |
H |
0.216 |
|
|
|
| 4 |
H |
0.216 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.659 |
0.000 |
0.000 |
| y |
0.000 |
-13.659 |
0.000 |
| z |
0.000 |
0.000 |
-6.896 |
|
| Traceless |
| | x | y | z |
| x |
-3.382 |
0.000 |
0.000 |
| y |
0.000 |
-3.382 |
0.000 |
| z |
0.000 |
0.000 |
6.763 |
|
| Polar |
| 3z2-r2 | 13.527 |
| x2-y2 | 0.000 |
| 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 |
2.737 |
0.000 |
0.000 |
| y |
0.000 |
2.737 |
0.000 |
| z |
0.000 |
0.000 |
4.579 |
<r2> (average value of r
2) Å
2
| <r2> |
16.948 |
| (<r2>)1/2 |
4.117 |