Vibrational Frequencies calculated at LSDA/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' |
3353 |
3311 |
0.30 |
|
|
|
| 2 |
A' |
3020 |
2983 |
33.77 |
|
|
|
| 3 |
A' |
2918 |
2882 |
55.44 |
|
|
|
| 4 |
A' |
1703 |
1682 |
23.02 |
|
|
|
| 5 |
A' |
1442 |
1425 |
4.63 |
|
|
|
| 6 |
A' |
1314 |
1298 |
44.18 |
|
|
|
| 7 |
A' |
1038 |
1025 |
40.05 |
|
|
|
| 8 |
A" |
1139 |
1125 |
49.97 |
|
|
|
| 9 |
A" |
1058 |
1045 |
19.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8492.0 cm
-1
Scaled (by 0.9877) Zero Point Vibrational Energy (zpe) 8387.6 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 LSDA/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.156 |
|
|
|
| 2 |
N |
-0.299 |
|
|
|
| 3 |
H |
0.119 |
|
|
|
| 4 |
H |
0.145 |
|
|
|
| 5 |
H |
0.191 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.414 |
1.313 |
0.000 |
1.930 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.594 |
2.029 |
0.000 |
| y |
2.029 |
-12.729 |
0.000 |
| z |
0.000 |
0.000 |
-13.564 |
|
| Traceless |
| | x | y | z |
| x |
1.553 |
2.029 |
0.000 |
| y |
2.029 |
-0.150 |
0.000 |
| z |
0.000 |
0.000 |
-1.402 |
|
| Polar |
| 3z2-r2 | -2.805 |
| x2-y2 | 1.135 |
| xy | 2.029 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.794 |
0.212 |
0.000 |
| y |
0.212 |
3.900 |
0.000 |
| z |
0.000 |
0.000 |
1.548 |
<r2> (average value of r
2) Å
2
| <r2> |
19.626 |
| (<r2>)1/2 |
4.430 |