Vibrational Frequencies calculated at PBEPBEultrafine/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 |
2310 |
2294 |
75.26 |
|
|
|
| 2 |
A1 |
1220 |
1212 |
137.78 |
|
|
|
| 3 |
A1 |
1101 |
1093 |
2.20 |
|
|
|
| 4 |
E |
2292 |
2277 |
103.70 |
|
|
|
| 4 |
E |
2292 |
2277 |
103.71 |
|
|
|
| 5 |
E |
1068 |
1060 |
22.07 |
|
|
|
| 5 |
E |
1068 |
1060 |
22.07 |
|
|
|
| 6 |
E |
800 |
795 |
19.22 |
|
|
|
| 6 |
E |
800 |
795 |
19.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6475.7 cm
-1
Scaled (by 0.9931) Zero Point Vibrational Energy (zpe) 6431.0 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 PBEPBEultrafine/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.448 |
|
|
|
| 2 |
O |
-0.450 |
|
|
|
| 3 |
H |
0.001 |
|
|
|
| 4 |
H |
0.001 |
|
|
|
| 5 |
H |
0.001 |
|
|
|
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 |
3.350 |
3.350 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.135 |
0.000 |
0.000 |
| y |
0.000 |
-19.135 |
0.000 |
| z |
0.000 |
0.000 |
-22.227 |
|
| Traceless |
| | x | y | z |
| x |
1.546 |
0.000 |
0.000 |
| y |
0.000 |
1.546 |
0.000 |
| z |
0.000 |
0.000 |
-3.092 |
|
| Polar |
| 3z2-r2 | -6.185 |
| 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 |
3.919 |
0.000 |
0.000 |
| y |
0.000 |
3.919 |
0.000 |
| z |
0.000 |
0.000 |
4.677 |
<r2> (average value of r
2) Å
2
| <r2> |
32.891 |
| (<r2>)1/2 |
5.735 |