Vibrational Frequencies calculated at B97D3/6-31+G**
| 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' |
1801 |
1770 |
314.15 |
|
|
|
| 2 |
A' |
1319 |
1297 |
278.25 |
|
|
|
| 3 |
A' |
781 |
767 |
140.44 |
|
|
|
| 4 |
A' |
727 |
714 |
13.60 |
|
|
|
| 5 |
A' |
498 |
490 |
24.47 |
|
|
|
| 6 |
A' |
370 |
363 |
31.14 |
|
|
|
| 7 |
A' |
217 |
213 |
0.27 |
|
|
|
| 8 |
A" |
663 |
651 |
7.34 |
|
|
|
| 9 |
A" |
130 |
127 |
0.56 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3252.0 cm
-1
Scaled (by 0.9828) Zero Point Vibrational Energy (zpe) 3196.0 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 B97D3/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cl |
0.176 |
|
|
|
| 2 |
O |
-0.127 |
|
|
|
| 3 |
N |
-0.063 |
|
|
|
| 4 |
O |
0.007 |
|
|
|
| 5 |
O |
0.007 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.777 |
-0.309 |
0.000 |
0.836 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.762 |
-0.459 |
0.000 |
| y |
-0.459 |
-35.721 |
0.000 |
| z |
0.000 |
0.000 |
-32.910 |
|
| Traceless |
| | x | y | z |
| x |
1.554 |
-0.459 |
0.000 |
| y |
-0.459 |
-2.886 |
0.000 |
| z |
0.000 |
0.000 |
1.332 |
|
| Polar |
| 3z2-r2 | 2.664 |
| x2-y2 | 2.959 |
| xy | -0.459 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.130 |
-0.581 |
0.000 |
| y |
-0.581 |
5.490 |
0.000 |
| z |
0.000 |
0.000 |
3.115 |
<r2> (average value of r
2) Å
2
| <r2> |
138.374 |
| (<r2>)1/2 |
11.763 |