Vibrational Frequencies calculated at B1B95/6-311G**
| 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 |
2433 |
2336 |
88.95 |
|
|
|
| 2 |
A1 |
1287 |
1236 |
212.57 |
|
|
|
| 3 |
A1 |
1175 |
1128 |
0.26 |
|
|
|
| 4 |
E |
2410 |
2314 |
132.09 |
|
|
|
| 4 |
E |
2410 |
2314 |
132.11 |
|
|
|
| 5 |
E |
1124 |
1079 |
38.10 |
|
|
|
| 5 |
E |
1124 |
1079 |
38.09 |
|
|
|
| 6 |
E |
863 |
828 |
37.13 |
|
|
|
| 6 |
E |
863 |
828 |
37.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6844.1 cm
-1
Scaled (by 0.9601) Zero Point Vibrational Energy (zpe) 6571.0 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 B1B95/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
P |
0.717 |
|
|
|
| 2 |
O |
-0.576 |
|
|
|
| 3 |
H |
-0.047 |
|
|
|
| 4 |
H |
-0.047 |
|
|
|
| 5 |
H |
-0.047 |
|
|
|
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 |
3.792 |
3.792 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.030 |
0.000 |
0.000 |
| y |
0.000 |
-19.030 |
0.000 |
| z |
0.000 |
0.000 |
-22.457 |
|
| Traceless |
| | x | y | z |
| x |
1.713 |
0.000 |
0.000 |
| y |
0.000 |
1.713 |
0.000 |
| z |
0.000 |
0.000 |
-3.427 |
|
| Polar |
| 3z2-r2 | -6.853 |
| 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 |
3.208 |
0.000 |
0.000 |
| y |
0.000 |
3.208 |
0.000 |
| z |
0.000 |
0.000 |
3.993 |
<r2> (average value of r
2) Å
2
| <r2> |
32.408 |
| (<r2>)1/2 |
5.693 |