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' |
3286 |
3136 |
1.87 |
|
|
|
| 2 |
A' |
3200 |
3054 |
5.16 |
|
|
|
| 3 |
A' |
3100 |
2958 |
4.23 |
|
|
|
| 4 |
A' |
1685 |
1608 |
1.63 |
|
|
|
| 5 |
A' |
1400 |
1336 |
7.03 |
|
|
|
| 6 |
A' |
1063 |
1014 |
9.84 |
|
|
|
| 7 |
A' |
724 |
691 |
22.08 |
|
|
|
| 8 |
A" |
927 |
885 |
76.96 |
|
|
|
| 9 |
A" |
836 |
798 |
7.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8110.2 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 7739.6 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 HSEh1PBE/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.126 |
|
|
|
| 2 |
C |
-0.312 |
|
|
|
| 3 |
H |
0.147 |
|
|
|
| 4 |
H |
0.143 |
|
|
|
| 5 |
H |
0.148 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.585 |
-0.250 |
0.000 |
0.636 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.926 |
-1.084 |
0.000 |
| y |
-1.084 |
-10.941 |
0.000 |
| z |
0.000 |
0.000 |
-14.249 |
|
| Traceless |
| | x | y | z |
| x |
0.669 |
-1.084 |
0.000 |
| y |
-1.084 |
2.146 |
0.000 |
| z |
0.000 |
0.000 |
-2.815 |
|
| Polar |
| 3z2-r2 | -5.631 |
| x2-y2 | -0.985 |
| xy | -1.084 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.484 |
-0.252 |
0.000 |
| y |
-0.252 |
4.443 |
0.000 |
| z |
0.000 |
0.000 |
1.328 |
<r2> (average value of r
2) Å
2
| <r2> |
20.155 |
| (<r2>)1/2 |
4.489 |