Vibrational Frequencies calculated at PBEPBE/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 |
2176 |
2146 |
155.80 |
|
|
|
| 2 |
A1 |
1127 |
1112 |
102.92 |
|
|
|
| 3 |
A1 |
929 |
917 |
16.72 |
|
|
|
| 4 |
E |
2143 |
2113 |
214.74 |
|
|
|
| 4 |
E |
2143 |
2113 |
214.76 |
|
|
|
| 5 |
E |
1012 |
998 |
33.19 |
|
|
|
| 5 |
E |
1012 |
998 |
33.18 |
|
|
|
| 6 |
E |
725 |
715 |
6.43 |
|
|
|
| 6 |
E |
725 |
715 |
6.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5996.2 cm
-1
Scaled (by 0.9862) Zero Point Vibrational Energy (zpe) 5913.5 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 PBEPBE/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.605 |
|
|
|
| 2 |
O |
-0.576 |
|
|
|
| 3 |
H |
-0.010 |
|
|
|
| 4 |
H |
-0.010 |
|
|
|
| 5 |
H |
-0.010 |
|
|
|
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 |
4.194 |
4.194 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.864 |
0.000 |
0.000 |
| y |
0.000 |
-19.864 |
0.000 |
| z |
0.000 |
0.000 |
-23.198 |
|
| Traceless |
| | x | y | z |
| x |
1.667 |
0.000 |
0.000 |
| y |
0.000 |
1.667 |
0.000 |
| z |
0.000 |
0.000 |
-3.334 |
|
| Polar |
| 3z2-r2 | -6.669 |
| 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 |
3.341 |
0.000 |
0.000 |
| y |
0.000 |
3.341 |
0.000 |
| z |
0.000 |
0.000 |
4.817 |
<r2> (average value of r
2) Å
2
| <r2> |
36.110 |
| (<r2>)1/2 |
6.009 |