Vibrational Frequencies calculated at HSEh1PBE/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' |
3263 |
3263 |
0.59 |
|
|
|
| 2 |
A' |
3166 |
3166 |
2.06 |
|
|
|
| 3 |
A' |
3069 |
3069 |
3.30 |
|
|
|
| 4 |
A' |
1664 |
1664 |
2.45 |
|
|
|
| 5 |
A' |
1388 |
1388 |
9.69 |
|
|
|
| 6 |
A' |
1044 |
1044 |
8.19 |
|
|
|
| 7 |
A' |
708 |
708 |
21.26 |
|
|
|
| 8 |
A" |
930 |
930 |
73.62 |
|
|
|
| 9 |
A" |
838 |
838 |
18.45 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8034.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8034.7 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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.249 |
|
|
|
| 2 |
C |
-0.193 |
|
|
|
| 3 |
H |
0.168 |
|
|
|
| 4 |
H |
0.132 |
|
|
|
| 5 |
H |
0.142 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.617 |
-0.320 |
0.000 |
0.695 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.411 |
-1.220 |
0.000 |
| y |
-1.220 |
-11.276 |
0.000 |
| z |
0.000 |
0.000 |
-14.927 |
|
| Traceless |
| | x | y | z |
| x |
0.690 |
-1.220 |
0.000 |
| y |
-1.220 |
2.393 |
0.000 |
| z |
0.000 |
0.000 |
-3.083 |
|
| Polar |
| 3z2-r2 | -6.166 |
| x2-y2 | -1.135 |
| xy | -1.220 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.354 |
-0.063 |
0.000 |
| y |
-0.063 |
5.073 |
0.000 |
| z |
0.000 |
0.000 |
3.095 |
<r2> (average value of r
2) Å
2
| <r2> |
20.373 |
| (<r2>)1/2 |
4.514 |