Vibrational Frequencies calculated at HF/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' |
3389 |
3065 |
3.21 |
|
|
|
| 2 |
A' |
3339 |
3020 |
13.42 |
|
|
|
| 3 |
A' |
3245 |
2935 |
11.18 |
|
|
|
| 4 |
A' |
1622 |
1467 |
2.93 |
|
|
|
| 5 |
A' |
1399 |
1265 |
4.06 |
|
|
|
| 6 |
A' |
1188 |
1074 |
8.23 |
|
|
|
| 7 |
A' |
824 |
745 |
13.82 |
|
|
|
| 8 |
A" |
955 |
864 |
80.59 |
|
|
|
| 9 |
A" |
884 |
800 |
4.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8422.0 cm
-1
Scaled (by 0.9044) Zero Point Vibrational Energy (zpe) 7616.8 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 HF/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.235 |
|
|
|
| 2 |
C |
-0.464 |
|
|
|
| 3 |
H |
0.239 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
| 5 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.582 |
-0.262 |
0.000 |
0.638 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
-0.582 |
-0.277 |
0.000 |
0.644 |
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.200 |
-1.082 |
0.000 |
| y |
-1.082 |
-11.504 |
0.000 |
| z |
0.000 |
0.000 |
-14.893 |
|
| Traceless |
| | x | y | z |
| x |
0.999 |
-1.082 |
0.000 |
| y |
-1.082 |
2.043 |
0.000 |
| z |
0.000 |
0.000 |
-3.042 |
|
| Polar |
| 3z2-r2 | -6.083 |
| x2-y2 | -0.696 |
| xy | -1.082 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.480 |
-0.223 |
0.000 |
| y |
-0.223 |
4.296 |
0.000 |
| z |
0.000 |
0.000 |
1.644 |
<r2> (average value of r
2) Å
2
| <r2> |
20.475 |
| (<r2>)1/2 |
4.525 |