Vibrational Frequencies calculated at B3LYP/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' |
3421 |
3307 |
2.13 |
|
|
|
| 2 |
A' |
3100 |
2997 |
41.98 |
|
|
|
| 3 |
A' |
3001 |
2902 |
55.24 |
|
|
|
| 4 |
A' |
1715 |
1658 |
22.04 |
|
|
|
| 5 |
A' |
1498 |
1449 |
6.04 |
|
|
|
| 6 |
A' |
1379 |
1333 |
44.54 |
|
|
|
| 7 |
A' |
1080 |
1044 |
35.06 |
|
|
|
| 8 |
A" |
1175 |
1136 |
48.65 |
|
|
|
| 9 |
A" |
1099 |
1063 |
15.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8733.9 cm
-1
Scaled (by 0.9668) Zero Point Vibrational Energy (zpe) 8444.0 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 B3LYP/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.076 |
|
|
|
| 2 |
N |
-0.296 |
|
|
|
| 3 |
H |
0.088 |
|
|
|
| 4 |
H |
0.113 |
|
|
|
| 5 |
H |
0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.391 |
1.375 |
0.000 |
1.956 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.621 |
1.979 |
0.000 |
| y |
1.979 |
-12.694 |
0.000 |
| z |
0.000 |
0.000 |
-13.451 |
|
| Traceless |
| | x | y | z |
| x |
1.451 |
1.979 |
0.000 |
| y |
1.979 |
-0.158 |
0.000 |
| z |
0.000 |
0.000 |
-1.293 |
|
| Polar |
| 3z2-r2 | -2.587 |
| x2-y2 | 1.073 |
| xy | 1.979 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.681 |
0.230 |
0.000 |
| y |
0.230 |
3.839 |
0.000 |
| z |
0.000 |
0.000 |
1.527 |
<r2> (average value of r
2) Å
2
| <r2> |
19.553 |
| (<r2>)1/2 |
4.422 |