Vibrational Frequencies calculated at B97D3/6-311+G(3df,2p)
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A' |
3161 |
3120 |
1.68 |
|
|
|
| 2 |
A' |
3071 |
3031 |
7.76 |
|
|
|
| 3 |
A' |
2271 |
2241 |
92.66 |
|
|
|
| 4 |
A' |
1419 |
1401 |
1.67 |
|
|
|
| 5 |
A' |
1016 |
1003 |
22.75 |
|
|
|
| 6 |
A' |
975 |
962 |
1.82 |
|
|
|
| 7 |
A' |
736 |
726 |
0.44 |
|
|
|
| 8 |
A" |
885 |
874 |
35.00 |
|
|
|
| 9 |
A" |
838 |
827 |
30.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7185.0 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 7091.6 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 B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.333 |
|
|
|
| 2 |
P |
0.037 |
|
|
|
| 3 |
H |
0.141 |
|
|
|
| 4 |
H |
0.138 |
|
|
|
| 5 |
H |
0.017 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.441 |
0.808 |
0.000 |
0.921 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.959 |
0.972 |
0.000 |
| y |
0.972 |
-19.545 |
0.000 |
| z |
0.000 |
0.000 |
-21.844 |
|
| Traceless |
| | x | y | z |
| x |
0.735 |
0.972 |
0.000 |
| y |
0.972 |
1.357 |
0.000 |
| z |
0.000 |
0.000 |
-2.092 |
|
| Polar |
| 3z2-r2 | -4.183 |
| x2-y2 | -0.414 |
| xy | 0.972 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.611 |
0.218 |
-0.000 |
| y |
0.218 |
7.843 |
0.001 |
| z |
-0.000 |
0.001 |
4.881 |
<r2> (average value of r
2) Å
2
| <r2> |
34.768 |
| (<r2>)1/2 |
5.896 |