Vibrational Frequencies calculated at wB97X-D/6-311G*
| 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' |
3253 |
3253 |
2.13 |
|
|
|
| 2 |
A' |
3171 |
3171 |
7.14 |
|
|
|
| 3 |
A' |
3075 |
3075 |
6.83 |
|
|
|
| 4 |
A' |
1672 |
1672 |
2.32 |
|
|
|
| 5 |
A' |
1405 |
1405 |
8.87 |
|
|
|
| 6 |
A' |
1073 |
1073 |
10.09 |
|
|
|
| 7 |
A' |
734 |
734 |
24.73 |
|
|
|
| 8 |
A" |
929 |
929 |
89.33 |
|
|
|
| 9 |
A" |
838 |
838 |
16.02 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8074.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8074.9 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 wB97X-D/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.234 |
|
|
|
| 2 |
C |
-0.464 |
|
|
|
| 3 |
H |
0.237 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
| 5 |
H |
0.235 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.665 |
-0.306 |
0.000 |
0.732 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.109 |
-1.231 |
0.000 |
| y |
-1.231 |
-11.123 |
0.000 |
| z |
0.000 |
0.000 |
-14.753 |
|
| Traceless |
| | x | y | z |
| x |
0.829 |
-1.231 |
0.000 |
| y |
-1.231 |
2.308 |
0.000 |
| z |
0.000 |
0.000 |
-3.137 |
|
| Polar |
| 3z2-r2 | -6.274 |
| x2-y2 | -0.986 |
| xy | -1.231 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.616 |
-0.183 |
0.000 |
| y |
-0.183 |
4.695 |
0.000 |
| z |
0.000 |
0.000 |
1.708 |
<r2> (average value of r
2) Å
2
| <r2> |
20.275 |
| (<r2>)1/2 |
4.503 |