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 |
A1 |
1933 |
1837 |
1.56 |
|
|
|
| 2 |
A1 |
1104 |
1049 |
44.75 |
|
|
|
| 3 |
A1 |
493 |
468 |
1.49 |
|
|
|
| 4 |
A1 |
291 |
276 |
0.59 |
|
|
|
| 5 |
A2 |
258 |
245 |
0.00 |
|
|
|
| 6 |
B1 |
145 |
138 |
0.09 |
|
|
|
| 7 |
B2 |
1874 |
1781 |
437.69 |
|
|
|
| 8 |
B2 |
793 |
753 |
16.84 |
|
|
|
| 9 |
B2 |
605 |
575 |
931.88 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3747.1 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 3561.3 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 |
O |
-0.324 |
|
|
|
| 2 |
N |
0.365 |
|
|
|
| 3 |
N |
0.365 |
|
|
|
| 4 |
O |
-0.203 |
|
|
|
| 5 |
O |
-0.203 |
|
|
|
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 |
-0.482 |
0.482 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.289 |
0.000 |
0.000 |
| y |
0.000 |
-28.420 |
0.000 |
| z |
0.000 |
0.000 |
-27.698 |
|
| Traceless |
| | x | y | z |
| x |
3.770 |
0.000 |
0.000 |
| y |
0.000 |
-2.427 |
0.000 |
| z |
0.000 |
0.000 |
-1.344 |
|
| Polar |
| 3z2-r2 | -2.687 |
| x2-y2 | 4.131 |
| 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 |
1.819 |
0.000 |
0.000 |
| y |
0.000 |
7.013 |
0.000 |
| z |
0.000 |
0.000 |
2.482 |
<r2> (average value of r
2) Å
2
| <r2> |
111.211 |
| (<r2>)1/2 |
10.546 |