Vibrational Frequencies calculated at M06-2X/3-21G*
| 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 |
3082 |
2919 |
11.19 |
|
|
|
| 2 |
A1 |
1446 |
1370 |
5.71 |
|
|
|
| 3 |
A1 |
727 |
689 |
26.44 |
|
|
|
| 4 |
E |
3176 |
3008 |
1.57 |
|
|
|
| 4 |
E |
3175 |
3008 |
1.59 |
|
|
|
| 5 |
E |
1547 |
1466 |
10.85 |
|
|
|
| 5 |
E |
1547 |
1466 |
10.81 |
|
|
|
| 6 |
E |
1061 |
1005 |
6.52 |
|
|
|
| 6 |
E |
1060 |
1004 |
6.54 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8410.6 cm
-1
Scaled (by 0.9472) Zero Point Vibrational Energy (zpe) 7966.6 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.668 |
|
|
|
| 2 |
Cl |
-0.079 |
|
|
|
| 3 |
H |
0.249 |
|
|
|
| 4 |
H |
0.249 |
|
|
|
| 5 |
H |
0.249 |
|
|
|
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 |
-2.114 |
2.114 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.919 |
0.000 |
0.000 |
| y |
0.000 |
-19.919 |
0.000 |
| z |
0.000 |
0.000 |
-18.121 |
|
| Traceless |
| | x | y | z |
| x |
-0.899 |
0.000 |
0.000 |
| y |
0.000 |
-0.899 |
0.000 |
| z |
0.000 |
0.000 |
1.797 |
|
| Polar |
| 3z2-r2 | 3.595 |
| 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 |
2.230 |
0.000 |
0.000 |
| y |
0.000 |
2.228 |
-0.001 |
| z |
0.000 |
-0.001 |
4.008 |
<r2> (average value of r
2) Å
2
| <r2> |
37.113 |
| (<r2>)1/2 |
6.092 |