Vibrational Frequencies calculated at HF/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 |
Σg |
3734 |
3372 |
0.00 |
56.44 |
0.18 |
0.31 |
| 2 |
Σg |
2209 |
1995 |
0.00 |
59.45 |
0.27 |
0.42 |
| 3 |
Σu |
3616 |
3264 |
98.41 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
899 |
811 |
0.00 |
6.22 |
0.75 |
0.86 |
| 4 |
Πg |
899 |
811 |
0.00 |
6.22 |
0.75 |
0.86 |
| 5 |
Πu |
892 |
805 |
141.10 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
892 |
805 |
141.10 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 6569.6 cm
-1
Scaled (by 0.9029) Zero Point Vibrational Energy (zpe) 5931.7 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 HF/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.320 |
|
|
|
| 2 |
C |
-0.320 |
|
|
|
| 3 |
H |
0.320 |
|
|
|
| 4 |
H |
0.320 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
0.000 |
0.000 |
0.000 |
0.000 |
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-13.406 |
0.000 |
0.000 |
| y |
0.000 |
-13.406 |
0.000 |
| z |
0.000 |
0.000 |
-6.953 |
|
| Traceless |
| | x | y | z |
| x |
-3.227 |
0.000 |
0.000 |
| y |
0.000 |
-3.227 |
0.000 |
| z |
0.000 |
0.000 |
6.453 |
|
| Polar |
| 3z2-r2 | 12.907 |
| x2-y2 | 0.000 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.970 |
0.000 |
0.000 |
| y |
0.000 |
0.970 |
0.000 |
| z |
0.000 |
0.000 |
4.147 |
<r2> (average value of r
2) Å
2
| <r2> |
16.753 |
| (<r2>)1/2 |
4.093 |