Vibrational Frequencies calculated at ROHF/3-21G
| 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' |
3417 |
3099 |
2.40 |
|
|
|
| 2 |
A' |
3364 |
3051 |
7.17 |
|
|
|
| 3 |
A' |
3285 |
2980 |
2.88 |
|
|
|
| 4 |
A' |
1798 |
1631 |
2.90 |
|
|
|
| 5 |
A' |
1560 |
1415 |
7.17 |
|
|
|
| 6 |
A' |
1240 |
1125 |
9.70 |
|
|
|
| 7 |
A' |
863 |
783 |
15.98 |
|
|
|
| 8 |
A" |
1100 |
998 |
80.97 |
|
|
|
| 9 |
A" |
1003 |
910 |
38.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8814.7 cm
-1
Scaled (by 0.907) Zero Point Vibrational Energy (zpe) 7994.9 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.185 |
|
|
|
| 2 |
C |
-0.506 |
|
|
|
| 3 |
H |
0.234 |
|
|
|
| 4 |
H |
0.225 |
|
|
|
| 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 |
| |
-0.612 |
-0.203 |
0.000 |
0.645 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.197 |
-1.078 |
0.001 |
| y |
-1.078 |
-11.380 |
-0.001 |
| z |
0.001 |
-0.001 |
-14.810 |
|
| Traceless |
| | x | y | z |
| x |
0.898 |
-1.078 |
0.001 |
| y |
-1.078 |
2.123 |
-0.001 |
| z |
0.001 |
-0.001 |
-3.022 |
|
| Polar |
| 3z2-r2 | -6.044 |
| x2-y2 | -0.817 |
| xy | -1.078 |
| 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> |
20.151 |
| (<r2>)1/2 |
4.489 |