Vibrational Frequencies calculated at B97D3/6-31G(2df,p)
| 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' |
3201 |
3201 |
2.10 |
|
|
|
| 2 |
A' |
3093 |
3093 |
7.57 |
|
|
|
| 3 |
A' |
2997 |
2997 |
8.14 |
|
|
|
| 4 |
A' |
1624 |
1624 |
1.12 |
|
|
|
| 5 |
A' |
1365 |
1365 |
6.29 |
|
|
|
| 6 |
A' |
1021 |
1021 |
11.44 |
|
|
|
| 7 |
A' |
687 |
687 |
25.07 |
|
|
|
| 8 |
A" |
893 |
893 |
61.14 |
|
|
|
| 9 |
A" |
776 |
776 |
6.50 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7828.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7828.3 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 B97D3/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.152 |
|
|
|
| 2 |
C |
-0.275 |
|
|
|
| 3 |
H |
0.156 |
|
|
|
| 4 |
H |
0.134 |
|
|
|
| 5 |
H |
0.137 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.553 |
-0.271 |
0.000 |
0.616 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.971 |
-1.051 |
0.000 |
| y |
-1.051 |
-10.998 |
0.000 |
| z |
0.000 |
0.000 |
-14.092 |
|
| Traceless |
| | x | y | z |
| x |
0.574 |
-1.051 |
0.000 |
| y |
-1.051 |
2.033 |
0.000 |
| z |
0.000 |
0.000 |
-2.607 |
|
| Polar |
| 3z2-r2 | -5.214 |
| x2-y2 | -0.972 |
| xy | -1.051 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.700 |
-0.227 |
0.000 |
| y |
-0.227 |
4.569 |
0.000 |
| z |
0.000 |
0.000 |
1.727 |
<r2> (average value of r
2) Å
2
| <r2> |
20.256 |
| (<r2>)1/2 |
4.501 |