Vibrational Frequencies calculated at B3LYPultrafine/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' |
3243 |
3243 |
0.57 |
|
|
|
| 2 |
A' |
3142 |
3142 |
3.28 |
|
|
|
| 3 |
A' |
3046 |
3046 |
4.68 |
|
|
|
| 4 |
A' |
1654 |
1654 |
2.10 |
|
|
|
| 5 |
A' |
1396 |
1396 |
8.40 |
|
|
|
| 6 |
A' |
1050 |
1050 |
8.24 |
|
|
|
| 7 |
A' |
711 |
711 |
22.68 |
|
|
|
| 8 |
A" |
929 |
929 |
71.64 |
|
|
|
| 9 |
A" |
821 |
821 |
21.25 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7995.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7995.5 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 B3LYPultrafine/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.170 |
|
|
|
| 2 |
C |
-0.195 |
|
|
|
| 3 |
H |
0.139 |
|
|
|
| 4 |
H |
0.108 |
|
|
|
| 5 |
H |
0.118 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.619 |
-0.321 |
0.000 |
0.697 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.498 |
-1.185 |
0.000 |
| y |
-1.185 |
-11.447 |
0.000 |
| z |
0.000 |
0.000 |
-14.867 |
|
| Traceless |
| | x | y | z |
| x |
0.659 |
-1.185 |
0.000 |
| y |
-1.185 |
2.235 |
0.000 |
| z |
0.000 |
0.000 |
-2.895 |
|
| Polar |
| 3z2-r2 | -5.789 |
| x2-y2 | -1.051 |
| xy | -1.185 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.075 |
-0.120 |
0.000 |
| y |
-0.120 |
5.089 |
0.000 |
| z |
0.000 |
0.000 |
2.558 |
<r2> (average value of r
2) Å
2
| <r2> |
20.423 |
| (<r2>)1/2 |
4.519 |