Vibrational Frequencies calculated at B2PLYP/6-31G
| 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' |
3292 |
3292 |
2.44 |
|
|
|
| 2 |
A' |
3208 |
3208 |
10.18 |
|
|
|
| 3 |
A' |
3105 |
3105 |
5.60 |
|
|
|
| 4 |
A' |
1695 |
1695 |
2.33 |
|
|
|
| 5 |
A' |
1464 |
1464 |
6.22 |
|
|
|
| 6 |
A' |
1109 |
1109 |
8.91 |
|
|
|
| 7 |
A' |
761 |
761 |
22.95 |
|
|
|
| 8 |
A" |
975 |
975 |
85.65 |
|
|
|
| 9 |
A" |
863 |
863 |
18.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8235.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8235.8 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 B2PLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.109 |
|
|
|
| 2 |
C |
-0.348 |
|
|
|
| 3 |
H |
0.150 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
| 5 |
H |
0.156 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.616 |
-0.246 |
0.000 |
0.664 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.198 |
-1.089 |
0.000 |
| y |
-1.089 |
-11.251 |
0.000 |
| z |
0.000 |
0.000 |
-14.403 |
|
| Traceless |
| | x | y | z |
| x |
0.628 |
-1.089 |
0.000 |
| y |
-1.089 |
2.050 |
0.000 |
| z |
0.000 |
0.000 |
-2.678 |
|
| Polar |
| 3z2-r2 | -5.356 |
| x2-y2 | -0.948 |
| xy | -1.089 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.358 |
-0.249 |
0.000 |
| y |
-0.249 |
4.408 |
0.000 |
| z |
0.000 |
0.000 |
1.122 |
<r2> (average value of r
2) Å
2
| <r2> |
20.435 |
| (<r2>)1/2 |
4.521 |