Vibrational Frequencies calculated at B3LYP/6-31G**
| 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 |
1301 |
1250 |
137.98 |
|
|
|
| 2 |
A1 |
458 |
440 |
19.96 |
|
|
|
| 3 |
A1 |
262 |
252 |
2.76 |
|
|
|
| 4 |
E |
573 |
551 |
249.41 |
|
|
|
| 4 |
E |
573 |
551 |
249.39 |
|
|
|
| 5 |
E |
321 |
309 |
8.40 |
|
|
|
| 5 |
E |
321 |
309 |
8.40 |
|
|
|
| 6 |
E |
181 |
174 |
0.02 |
|
|
|
| 6 |
E |
181 |
174 |
0.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2086.2 cm
-1
Scaled (by 0.9608) Zero Point Vibrational Energy (zpe) 2004.4 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 B3LYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.685 |
|
|
|
| 2 |
O |
-0.415 |
|
|
|
| 3 |
Cl |
-0.090 |
|
|
|
| 4 |
Cl |
-0.090 |
|
|
|
| 5 |
Cl |
-0.090 |
|
|
|
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 |
-2.020 |
2.020 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-54.192 |
0.000 |
0.000 |
| y |
0.000 |
-54.192 |
0.000 |
| z |
0.000 |
0.000 |
-60.437 |
|
| Traceless |
| | x | y | z |
| x |
3.123 |
0.000 |
0.000 |
| y |
0.000 |
3.123 |
0.000 |
| z |
0.000 |
0.000 |
-6.245 |
|
| Polar |
| 3z2-r2 | -12.490 |
| 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 |
8.135 |
0.000 |
0.000 |
| y |
0.000 |
8.135 |
0.000 |
| z |
0.000 |
0.000 |
6.443 |
<r2> (average value of r
2) Å
2
| <r2> |
250.628 |
| (<r2>)1/2 |
15.831 |