Vibrational Frequencies calculated at B97D3/aug-cc-pVTZ
| 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' |
1791 |
1764 |
319.13 |
|
|
|
| 2 |
A' |
1308 |
1288 |
275.13 |
|
|
|
| 3 |
A' |
795 |
783 |
126.74 |
|
|
|
| 4 |
A' |
742 |
731 |
25.00 |
|
|
|
| 5 |
A' |
509 |
501 |
26.39 |
|
|
|
| 6 |
A' |
366 |
361 |
33.20 |
|
|
|
| 7 |
A' |
220 |
217 |
0.38 |
|
|
|
| 8 |
A" |
670 |
660 |
6.78 |
|
|
|
| 9 |
A" |
126 |
124 |
0.33 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3263.6 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 3213.7 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/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cl |
0.178 |
|
|
|
| 2 |
O |
-0.397 |
|
|
|
| 3 |
N |
1.052 |
|
|
|
| 4 |
O |
-0.406 |
|
|
|
| 5 |
O |
-0.427 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.509 |
-0.330 |
0.000 |
0.607 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.804 |
-0.527 |
0.000 |
| y |
-0.527 |
-35.230 |
0.000 |
| z |
0.000 |
0.000 |
-32.673 |
|
| Traceless |
| | x | y | z |
| x |
1.148 |
-0.527 |
0.000 |
| y |
-0.527 |
-2.491 |
0.000 |
| z |
0.000 |
0.000 |
1.343 |
|
| Polar |
| 3z2-r2 | 2.687 |
| x2-y2 | 2.426 |
| xy | -0.527 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
9.651 |
-0.777 |
0.000 |
| y |
-0.777 |
6.220 |
0.000 |
| z |
0.000 |
0.000 |
4.046 |
<r2> (average value of r
2) Å
2
| <r2> |
137.029 |
| (<r2>)1/2 |
11.706 |