Vibrational Frequencies calculated at B97D3/aug-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 |
2339 |
2303 |
89.10 |
|
|
|
| 2 |
A1 |
1212 |
1193 |
158.90 |
|
|
|
| 3 |
A1 |
1112 |
1095 |
0.05 |
|
|
|
| 4 |
E |
2323 |
2287 |
92.35 |
|
|
|
| 4 |
E |
2323 |
2287 |
92.33 |
|
|
|
| 5 |
E |
1091 |
1074 |
19.68 |
|
|
|
| 5 |
E |
1091 |
1074 |
19.68 |
|
|
|
| 6 |
E |
811 |
799 |
18.27 |
|
|
|
| 6 |
E |
811 |
799 |
18.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6556.3 cm
-1
Scaled (by 0.9847) Zero Point Vibrational Energy (zpe) 6456.0 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 B97D3/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.721 |
|
|
|
| 2 |
O |
-0.782 |
|
|
|
| 3 |
H |
0.020 |
|
|
|
| 4 |
H |
0.020 |
|
|
|
| 5 |
H |
0.020 |
|
|
|
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 |
3.549 |
3.549 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.092 |
0.000 |
0.000 |
| y |
0.000 |
-19.092 |
0.000 |
| z |
0.000 |
0.000 |
-22.745 |
|
| Traceless |
| | x | y | z |
| x |
1.826 |
0.000 |
0.000 |
| y |
0.000 |
1.826 |
0.000 |
| z |
0.000 |
0.000 |
-3.653 |
|
| Polar |
| 3z2-r2 | -7.306 |
| 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 |
4.414 |
0.000 |
0.000 |
| y |
0.000 |
4.414 |
-0.000 |
| z |
0.000 |
-0.000 |
5.328 |
<r2> (average value of r
2) Å
2
| <r2> |
32.817 |
| (<r2>)1/2 |
5.729 |