Vibrational Frequencies calculated at HF/Def2TZVPP
| 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 |
1541 |
1397 |
329.11 |
|
|
|
| 2 |
A1 |
972 |
881 |
39.65 |
|
|
|
| 3 |
A1 |
523 |
474 |
43.40 |
|
|
|
| 4 |
E |
1091 |
989 |
276.64 |
|
|
|
| 4 |
E |
1091 |
989 |
276.64 |
|
|
|
| 5 |
E |
523 |
474 |
63.40 |
|
|
|
| 5 |
E |
523 |
474 |
63.40 |
|
|
|
| 6 |
E |
365 |
331 |
0.66 |
|
|
|
| 6 |
E |
365 |
331 |
0.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3497.6 cm
-1
Scaled (by 0.9064) Zero Point Vibrational Energy (zpe) 3170.2 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
1.430 |
|
|
|
| 2 |
O |
-0.578 |
|
|
|
| 3 |
F |
-0.284 |
|
|
|
| 4 |
F |
-0.284 |
|
|
|
| 5 |
F |
-0.284 |
|
|
|
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 |
-2.158 |
2.158 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-31.313 |
0.000 |
0.000 |
| y |
0.000 |
-31.313 |
0.000 |
| z |
0.000 |
0.000 |
-36.748 |
|
| Traceless |
| | x | y | z |
| x |
2.717 |
0.000 |
0.000 |
| y |
0.000 |
2.717 |
0.000 |
| z |
0.000 |
0.000 |
-5.435 |
|
| Polar |
| 3z2-r2 | -10.870 |
| 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 |
2.722 |
0.000 |
0.000 |
| y |
0.000 |
2.722 |
0.000 |
| z |
0.000 |
0.000 |
3.148 |
<r2> (average value of r
2) Å
2
| <r2> |
96.558 |
| (<r2>)1/2 |
9.826 |