Vibrational Frequencies calculated at M06-2X/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 |
A |
3917 |
3917 |
68.39 |
|
|
|
| 2 |
A |
3274 |
3274 |
12.90 |
|
|
|
| 3 |
A |
3133 |
3133 |
20.01 |
|
|
|
| 4 |
A |
1503 |
1503 |
9.95 |
|
|
|
| 5 |
A |
1370 |
1370 |
29.36 |
|
|
|
| 6 |
A |
1244 |
1244 |
113.44 |
|
|
|
| 7 |
A |
1072 |
1072 |
47.64 |
|
|
|
| 8 |
A |
636 |
636 |
72.51 |
|
|
|
| 9 |
A |
424 |
424 |
86.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8285.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8285.6 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 M06-2X/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.172 |
|
|
|
| 2 |
O |
-0.344 |
|
|
|
| 3 |
H |
0.134 |
|
|
|
| 4 |
H |
0.115 |
|
|
|
| 5 |
H |
0.267 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.054 |
1.564 |
0.223 |
1.581 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.538 |
-2.166 |
0.692 |
| y |
-2.166 |
-10.962 |
-0.034 |
| z |
0.692 |
-0.034 |
-14.118 |
|
| Traceless |
| | x | y | z |
| x |
1.002 |
-2.166 |
0.692 |
| y |
-2.166 |
1.866 |
-0.034 |
| z |
0.692 |
-0.034 |
-2.867 |
|
| Polar |
| 3z2-r2 | -5.735 |
| x2-y2 | -0.576 |
| xy | -2.166 |
| xz | 0.692 |
| yz | -0.034 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.759 |
-0.133 |
0.037 |
| y |
-0.133 |
2.308 |
0.000 |
| z |
0.037 |
0.000 |
1.605 |
<r2> (average value of r
2) Å
2
| <r2> |
20.431 |
| (<r2>)1/2 |
4.520 |