Vibrational Frequencies calculated at PBE1PBE/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 |
3641 |
3490 |
21.00 |
|
|
|
| 2 |
A |
1307 |
1253 |
0.09 |
|
|
|
| 3 |
A |
930 |
891 |
11.57 |
|
|
|
| 4 |
A |
747 |
716 |
117.23 |
|
|
|
| 5 |
A |
546 |
523 |
0.35 |
|
|
|
| 6 |
B |
3640 |
3489 |
100.93 |
|
|
|
| 7 |
B |
2275 |
2181 |
617.35 |
|
|
|
| 8 |
B |
933 |
894 |
467.70 |
|
|
|
| 9 |
B |
548 |
525 |
86.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7283.0 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 6980.8 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 PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.556 |
|
|
|
| 2 |
N |
-0.621 |
|
|
|
| 3 |
N |
-0.621 |
|
|
|
| 4 |
H |
0.343 |
|
|
|
| 5 |
H |
0.343 |
|
|
|
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 |
2.264 |
2.264 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.597 |
4.458 |
0.000 |
| y |
4.458 |
-16.113 |
0.000 |
| z |
0.000 |
0.000 |
-17.190 |
|
| Traceless |
| | x | y | z |
| x |
0.054 |
4.458 |
0.000 |
| y |
4.458 |
0.780 |
0.000 |
| z |
0.000 |
0.000 |
-0.835 |
|
| Polar |
| 3z2-r2 | -1.670 |
| x2-y2 | -0.484 |
| xy | 4.458 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.968 |
0.321 |
0.000 |
| y |
0.321 |
5.938 |
0.000 |
| z |
0.000 |
0.000 |
1.936 |
<r2> (average value of r
2) Å
2
| <r2> |
38.626 |
| (<r2>)1/2 |
6.215 |