Vibrational Frequencies calculated at B3PW91/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 |
2389 |
2305 |
77.63 |
|
|
|
| 2 |
A1 |
1236 |
1192 |
169.08 |
|
|
|
| 3 |
A1 |
1124 |
1084 |
0.01 |
|
|
|
| 4 |
E |
2369 |
2286 |
126.37 |
|
|
|
| 4 |
E |
2369 |
2286 |
126.38 |
|
|
|
| 5 |
E |
1100 |
1061 |
31.35 |
|
|
|
| 5 |
E |
1100 |
1061 |
31.35 |
|
|
|
| 6 |
E |
822 |
793 |
25.53 |
|
|
|
| 6 |
E |
822 |
793 |
25.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6664.1 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 6430.9 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 B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.488 |
|
|
|
| 2 |
O |
-0.464 |
|
|
|
| 3 |
H |
-0.008 |
|
|
|
| 4 |
H |
-0.008 |
|
|
|
| 5 |
H |
-0.008 |
|
|
|
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 |
3.509 |
3.509 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.906 |
0.000 |
0.000 |
| y |
0.000 |
-18.906 |
0.000 |
| z |
0.000 |
0.000 |
-21.824 |
|
| Traceless |
| | x | y | z |
| x |
1.459 |
0.000 |
0.000 |
| y |
0.000 |
1.459 |
0.000 |
| z |
0.000 |
0.000 |
-2.918 |
|
| Polar |
| 3z2-r2 | -5.836 |
| 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 |
3.382 |
0.000 |
0.000 |
| y |
0.000 |
3.382 |
0.000 |
| z |
0.000 |
0.000 |
4.096 |
<r2> (average value of r
2) Å
2
| <r2> |
32.920 |
| (<r2>)1/2 |
5.738 |