Vibrational Frequencies calculated at HF/cc-pVDZ
| 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 |
1380 |
1253 |
222.56 |
|
|
|
| 2 |
A1 |
510 |
463 |
17.32 |
|
|
|
| 3 |
A1 |
280 |
254 |
3.51 |
|
|
|
| 4 |
E |
625 |
568 |
291.89 |
|
|
|
| 4 |
E |
625 |
568 |
291.89 |
|
|
|
| 5 |
E |
353 |
321 |
19.27 |
|
|
|
| 5 |
E |
353 |
321 |
19.27 |
|
|
|
| 6 |
E |
200 |
182 |
0.00 |
|
|
|
| 6 |
E |
200 |
182 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2263.4 cm
-1
Scaled (by 0.908) Zero Point Vibrational Energy (zpe) 2055.2 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 HF/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.967 |
0.671 |
|
|
| 2 |
O |
-0.511 |
-0.470 |
|
|
| 3 |
Cl |
-0.152 |
-0.067 |
|
|
| 4 |
Cl |
-0.152 |
-0.067 |
|
|
| 5 |
Cl |
-0.152 |
-0.067 |
|
|
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 |
-2.517 |
2.517 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-54.113 |
0.000 |
0.000 |
| y |
0.000 |
-54.113 |
0.000 |
| z |
0.000 |
0.000 |
-62.080 |
|
| Traceless |
| | x | y | z |
| x |
3.984 |
0.000 |
0.000 |
| y |
0.000 |
3.984 |
0.000 |
| z |
0.000 |
0.000 |
-7.967 |
|
| Polar |
| 3z2-r2 | -15.935 |
| 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 |
7.321 |
0.000 |
0.000 |
| y |
0.000 |
7.321 |
0.000 |
| z |
0.000 |
0.000 |
5.759 |
<r2> (average value of r
2) Å
2
| <r2> |
246.074 |
| (<r2>)1/2 |
15.687 |