Vibrational Frequencies calculated at HSEh1PBE/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 |
A' |
3274 |
3113 |
0.99 |
|
|
|
| 2 |
A' |
3180 |
3024 |
4.57 |
|
|
|
| 3 |
A' |
2385 |
2269 |
136.08 |
|
|
|
| 4 |
A' |
1483 |
1410 |
0.79 |
|
|
|
| 5 |
A' |
1052 |
1000 |
37.97 |
|
|
|
| 6 |
A' |
1022 |
972 |
0.79 |
|
|
|
| 7 |
A' |
757 |
720 |
0.24 |
|
|
|
| 8 |
A" |
929 |
884 |
51.94 |
|
|
|
| 9 |
A" |
870 |
828 |
32.47 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7476.5 cm
-1
Scaled (by 0.951) Zero Point Vibrational Energy (zpe) 7110.2 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 HSEh1PBE/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.524 |
|
|
|
| 2 |
P |
0.122 |
|
|
|
| 3 |
H |
0.210 |
|
|
|
| 4 |
H |
0.207 |
|
|
|
| 5 |
H |
-0.015 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.589 |
1.089 |
0.000 |
1.238 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.541 |
1.130 |
0.000 |
| y |
1.130 |
-19.171 |
0.000 |
| z |
0.000 |
0.000 |
-21.419 |
|
| Traceless |
| | x | y | z |
| x |
0.755 |
1.130 |
0.000 |
| y |
1.130 |
1.308 |
0.000 |
| z |
0.000 |
0.000 |
-2.063 |
|
| Polar |
| 3z2-r2 | -4.126 |
| x2-y2 | -0.369 |
| xy | 1.130 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.358 |
0.327 |
0.000 |
| y |
0.327 |
6.635 |
0.000 |
| z |
0.000 |
0.000 |
2.901 |
<r2> (average value of r
2) Å
2
| <r2> |
34.461 |
| (<r2>)1/2 |
5.870 |