Vibrational Frequencies calculated at PBEPBEultrafine/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 |
A' |
3148 |
3113 |
0.57 |
|
|
|
| 2 |
A' |
3061 |
3026 |
4.70 |
|
|
|
| 3 |
A' |
2272 |
2247 |
82.84 |
|
|
|
| 4 |
A' |
1396 |
1381 |
2.01 |
|
|
|
| 5 |
A' |
997 |
986 |
18.20 |
|
|
|
| 6 |
A' |
975 |
964 |
4.13 |
|
|
|
| 7 |
A' |
721 |
713 |
0.39 |
|
|
|
| 8 |
A" |
877 |
867 |
34.60 |
|
|
|
| 9 |
A" |
829 |
819 |
29.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7137.3 cm
-1
Scaled (by 0.9888) Zero Point Vibrational Energy (zpe) 7057.4 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 PBEPBEultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.766 |
|
|
|
| 2 |
P |
0.104 |
|
|
|
| 3 |
H |
0.307 |
|
|
|
| 4 |
H |
0.324 |
|
|
|
| 5 |
H |
0.032 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.449 |
0.804 |
0.000 |
0.921 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.979 |
0.969 |
0.000 |
| y |
0.969 |
-19.638 |
0.000 |
| z |
0.000 |
0.000 |
-21.945 |
|
| Traceless |
| | x | y | z |
| x |
0.812 |
0.969 |
0.000 |
| y |
0.969 |
1.324 |
0.000 |
| z |
0.000 |
0.000 |
-2.136 |
|
| Polar |
| 3z2-r2 | -4.272 |
| x2-y2 | -0.341 |
| xy | 0.969 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.887 |
0.229 |
0.000 |
| y |
0.229 |
7.989 |
0.000 |
| z |
0.000 |
0.000 |
5.082 |
<r2> (average value of r
2) Å
2
| <r2> |
34.974 |
| (<r2>)1/2 |
5.914 |