Vibrational Frequencies calculated at ROHF/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' |
3392 |
3392 |
1.97 |
|
|
|
| 2 |
A' |
3350 |
3350 |
8.25 |
|
|
|
| 3 |
A' |
3264 |
3264 |
5.33 |
|
|
|
| 4 |
A' |
1795 |
1795 |
1.85 |
|
|
|
| 5 |
A' |
1513 |
1513 |
6.14 |
|
|
|
| 6 |
A' |
1202 |
1202 |
9.91 |
|
|
|
| 7 |
A' |
824 |
824 |
12.79 |
|
|
|
| 8 |
A" |
1059 |
1059 |
62.55 |
|
|
|
| 9 |
A" |
971 |
971 |
16.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8684.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8684.3 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 ROHF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.168 |
|
|
|
| 2 |
C |
-0.332 |
|
|
|
| 3 |
H |
0.182 |
|
|
|
| 4 |
H |
0.158 |
|
|
|
| 5 |
H |
0.161 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.551 |
-0.205 |
0.000 |
0.588 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.018 |
-1.031 |
0.001 |
| y |
-1.031 |
-11.148 |
-0.001 |
| z |
0.001 |
-0.001 |
-14.430 |
|
| Traceless |
| | x | y | z |
| x |
0.771 |
-1.031 |
0.001 |
| y |
-1.031 |
2.076 |
-0.001 |
| z |
0.001 |
-0.001 |
-2.847 |
|
| Polar |
| 3z2-r2 | -5.693 |
| x2-y2 | -0.870 |
| xy | -1.031 |
| xz | 0.001 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
0.000 |
0.000 |
0.000 |
| y |
0.000 |
0.000 |
0.000 |
| z |
0.000 |
0.000 |
0.000 |
<r2> (average value of r
2) Å
2
| <r2> |
19.985 |
| (<r2>)1/2 |
4.470 |