Vibrational Frequencies calculated at HSEh1PBE/Def2TZVPP
| 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' |
3266 |
3266 |
0.66 |
|
|
|
| 2 |
A' |
3171 |
3171 |
2.46 |
|
|
|
| 3 |
A' |
3074 |
3074 |
3.59 |
|
|
|
| 4 |
A' |
1667 |
1667 |
2.24 |
|
|
|
| 5 |
A' |
1389 |
1389 |
9.28 |
|
|
|
| 6 |
A' |
1046 |
1046 |
8.31 |
|
|
|
| 7 |
A' |
709 |
709 |
22.07 |
|
|
|
| 8 |
A" |
930 |
930 |
74.24 |
|
|
|
| 9 |
A" |
838 |
838 |
18.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8044.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8044.3 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/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.164 |
|
|
|
| 2 |
C |
-0.173 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 4 |
H |
0.099 |
|
|
|
| 5 |
H |
0.109 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.619 |
-0.309 |
0.000 |
0.692 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.346 |
-1.196 |
0.000 |
| y |
-1.196 |
-11.285 |
0.000 |
| z |
0.000 |
0.000 |
-14.804 |
|
| Traceless |
| | x | y | z |
| x |
0.699 |
-1.196 |
0.000 |
| y |
-1.196 |
2.290 |
0.000 |
| z |
0.000 |
0.000 |
-2.989 |
|
| Polar |
| 3z2-r2 | -5.977 |
| x2-y2 | -1.061 |
| xy | -1.196 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.047 |
-0.124 |
0.000 |
| y |
-0.124 |
5.027 |
0.000 |
| z |
0.000 |
0.000 |
2.550 |
<r2> (average value of r
2) Å
2
| <r2> |
20.335 |
| (<r2>)1/2 |
4.509 |