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' |
1880 |
1880 |
444.75 |
|
|
|
| 2 |
A' |
1413 |
1413 |
311.23 |
|
|
|
| 3 |
A' |
876 |
876 |
261.89 |
|
|
|
| 4 |
A' |
861 |
861 |
4.96 |
|
|
|
| 5 |
A' |
665 |
665 |
49.13 |
|
|
|
| 6 |
A' |
491 |
491 |
2.98 |
|
|
|
| 7 |
A' |
278 |
278 |
0.03 |
|
|
|
| 8 |
A" |
778 |
778 |
18.66 |
|
|
|
| 9 |
A" |
113 |
113 |
0.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3677.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3677.0 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 |
Cl |
0.235 |
|
|
|
| 2 |
O |
-0.320 |
|
|
|
| 3 |
N |
0.505 |
|
|
|
| 4 |
O |
-0.212 |
|
|
|
| 5 |
O |
-0.208 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.337 |
-0.041 |
0.000 |
1.338 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-33.263 |
-0.218 |
0.000 |
| y |
-0.218 |
-36.456 |
0.000 |
| z |
0.000 |
0.000 |
-32.818 |
|
| Traceless |
| | x | y | z |
| x |
1.374 |
-0.218 |
0.000 |
| y |
-0.218 |
-3.416 |
0.000 |
| z |
0.000 |
0.000 |
2.041 |
|
| Polar |
| 3z2-r2 | 4.083 |
| x2-y2 | 3.193 |
| xy | -0.218 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.106 |
0.140 |
0.000 |
| y |
0.140 |
3.938 |
0.000 |
| z |
0.000 |
0.000 |
1.800 |
<r2> (average value of r
2) Å
2
| <r2> |
130.993 |
| (<r2>)1/2 |
11.445 |