Vibrational Frequencies calculated at B3LYP/6-311+G(3df,2p)
| 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 |
3600 |
3482 |
25.11 |
|
|
|
| 2 |
A |
1289 |
1247 |
0.00 |
|
|
|
| 3 |
A |
911 |
881 |
13.63 |
|
|
|
| 4 |
A |
716 |
693 |
91.81 |
|
|
|
| 5 |
A |
544 |
526 |
0.40 |
|
|
|
| 6 |
B |
3598 |
3479 |
148.84 |
|
|
|
| 7 |
B |
2221 |
2148 |
700.43 |
|
|
|
| 8 |
B |
911 |
880 |
442.93 |
|
|
|
| 9 |
B |
548 |
530 |
74.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7168.8 cm
-1
Scaled (by 0.967) Zero Point Vibrational Energy (zpe) 6932.2 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/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.255 |
|
|
|
| 2 |
N |
-0.854 |
|
|
|
| 3 |
N |
-0.854 |
|
|
|
| 4 |
H |
0.226 |
|
|
|
| 5 |
H |
0.226 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.970 |
1.970 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.149 |
4.136 |
0.000 |
| y |
4.136 |
-16.487 |
0.000 |
| z |
0.000 |
0.000 |
-17.652 |
|
| Traceless |
| | x | y | z |
| x |
-0.080 |
4.136 |
0.000 |
| y |
4.136 |
0.914 |
0.000 |
| z |
0.000 |
0.000 |
-0.834 |
|
| Polar |
| 3z2-r2 | -1.668 |
| x2-y2 | -0.662 |
| xy | 4.136 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.021 |
0.232 |
0.000 |
| y |
0.232 |
6.819 |
0.000 |
| z |
0.000 |
0.000 |
2.994 |
<r2> (average value of r
2) Å
2
| <r2> |
38.955 |
| (<r2>)1/2 |
6.241 |