Vibrational Frequencies calculated at M06-2X/6-31G**
| 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 |
3556 |
3380 |
0.00 |
68.43 |
0.22 |
0.36 |
| 2 |
Σg |
2121 |
2016 |
0.00 |
53.67 |
0.26 |
0.41 |
| 3 |
Σu |
3451 |
3280 |
93.08 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
653 |
621 |
0.00 |
0.87 |
0.75 |
0.86 |
| 4 |
Πg |
653 |
621 |
0.00 |
0.87 |
0.75 |
0.86 |
| 5 |
Πu |
797 |
757 |
84.58 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
797 |
757 |
84.58 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 6013.8 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 5715.5 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 M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
C |
-0.185 |
|
|
|
| 3 |
H |
0.185 |
|
|
|
| 4 |
H |
0.185 |
|
|
|
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 |
-13.101 |
0.000 |
0.000 |
| y |
0.000 |
-13.101 |
0.000 |
| z |
0.000 |
0.000 |
-6.668 |
|
| Traceless |
| | x | y | z |
| x |
-3.217 |
0.000 |
0.000 |
| y |
0.000 |
-3.217 |
0.000 |
| z |
0.000 |
0.000 |
6.433 |
|
| Polar |
| 3z2-r2 | 12.866 |
| 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 |
1.180 |
0.000 |
0.000 |
| y |
0.000 |
1.180 |
0.000 |
| z |
0.000 |
0.000 |
4.204 |
<r2> (average value of r
2) Å
2
| <r2> |
16.745 |
| (<r2>)1/2 |
4.092 |