Vibrational Frequencies calculated at wB97X-D/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 |
1370 |
1298 |
129.44 |
|
|
|
| 2 |
A1 |
496 |
470 |
20.84 |
|
|
|
| 3 |
A1 |
279 |
265 |
4.02 |
|
|
|
| 4 |
E |
608 |
576 |
257.28 |
|
|
|
| 4 |
E |
608 |
576 |
257.60 |
|
|
|
| 5 |
E |
339 |
321 |
10.14 |
|
|
|
| 5 |
E |
339 |
321 |
10.15 |
|
|
|
| 6 |
E |
197 |
187 |
0.11 |
|
|
|
| 6 |
E |
197 |
187 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2215.9 cm
-1
Scaled (by 0.9478) Zero Point Vibrational Energy (zpe) 2100.2 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 wB97X-D/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.705 |
|
|
|
| 2 |
O |
-0.354 |
|
|
|
| 3 |
Cl |
-0.117 |
|
|
|
| 4 |
Cl |
-0.117 |
|
|
|
| 5 |
Cl |
-0.117 |
|
|
|
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 |
-1.854 |
1.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-54.597 |
0.000 |
0.000 |
| y |
0.000 |
-54.597 |
0.000 |
| z |
0.000 |
0.000 |
-60.385 |
|
| Traceless |
| | x | y | z |
| x |
2.894 |
0.000 |
0.000 |
| y |
0.000 |
2.894 |
0.000 |
| z |
0.000 |
0.000 |
-5.788 |
|
| Polar |
| 3z2-r2 | -11.576 |
| 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 |
7.224 |
0.000 |
0.000 |
| y |
0.000 |
7.228 |
0.000 |
| z |
0.000 |
0.000 |
5.745 |
<r2> (average value of r
2) Å
2
| <r2> |
243.372 |
| (<r2>)1/2 |
15.600 |