Vibrational Frequencies calculated at B97D3/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 |
A1 |
1279 |
1261 |
119.27 |
|
|
|
| 2 |
A1 |
440 |
434 |
15.59 |
|
|
|
| 3 |
A1 |
249 |
246 |
0.67 |
|
|
|
| 4 |
E |
541 |
533 |
227.13 |
|
|
|
| 4 |
E |
541 |
533 |
227.09 |
|
|
|
| 5 |
E |
310 |
305 |
5.06 |
|
|
|
| 5 |
E |
310 |
305 |
5.06 |
|
|
|
| 6 |
E |
176 |
173 |
0.05 |
|
|
|
| 6 |
E |
176 |
173 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2009.8 cm
-1
Scaled (by 0.986) Zero Point Vibrational Energy (zpe) 1981.7 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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.710 |
|
|
|
| 2 |
O |
-0.376 |
|
|
|
| 3 |
Cl |
-0.111 |
|
|
|
| 4 |
Cl |
-0.111 |
|
|
|
| 5 |
Cl |
-0.111 |
|
|
|
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 |
-2.077 |
2.077 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.667 |
0.000 |
0.000 |
| y |
0.000 |
-52.667 |
0.000 |
| z |
0.000 |
0.000 |
-59.612 |
|
| Traceless |
| | x | y | z |
| x |
3.472 |
0.000 |
0.000 |
| y |
0.000 |
3.472 |
0.000 |
| z |
0.000 |
0.000 |
-6.945 |
|
| Polar |
| 3z2-r2 | -13.889 |
| 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 |
9.563 |
0.000 |
0.000 |
| y |
0.000 |
9.562 |
0.000 |
| z |
0.000 |
0.000 |
7.843 |
<r2> (average value of r
2) Å
2
| <r2> |
249.825 |
| (<r2>)1/2 |
15.806 |