Vibrational Frequencies calculated at wB97X-D/TZVP
| 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' |
3253 |
3107 |
0.52 |
|
|
|
| 2 |
A' |
3158 |
3016 |
3.27 |
|
|
|
| 3 |
A' |
2338 |
2232 |
104.88 |
|
|
|
| 4 |
A' |
1468 |
1402 |
3.47 |
|
|
|
| 5 |
A' |
1054 |
1007 |
27.23 |
|
|
|
| 6 |
A' |
1032 |
985 |
3.52 |
|
|
|
| 7 |
A' |
768 |
734 |
0.24 |
|
|
|
| 8 |
A" |
933 |
891 |
67.46 |
|
|
|
| 9 |
A" |
875 |
836 |
19.06 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7440.0 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 7105.2 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 wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.433 |
|
|
|
| 2 |
P |
0.136 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.159 |
|
|
|
| 5 |
H |
-0.027 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.568 |
0.831 |
0.000 |
1.006 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.724 |
1.081 |
0.000 |
| y |
1.081 |
-19.500 |
0.000 |
| z |
0.000 |
0.000 |
-21.676 |
|
| Traceless |
| | x | y | z |
| x |
0.864 |
1.081 |
0.000 |
| y |
1.081 |
1.200 |
0.000 |
| z |
0.000 |
0.000 |
-2.064 |
|
| Polar |
| 3z2-r2 | -4.129 |
| x2-y2 | -0.224 |
| xy | 1.081 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.904 |
0.304 |
0.000 |
| y |
0.304 |
7.566 |
0.000 |
| z |
0.000 |
0.000 |
3.237 |
<r2> (average value of r
2) Å
2
| <r2> |
34.498 |
| (<r2>)1/2 |
5.873 |