Vibrational Frequencies calculated at BLYP/aug-cc-pVTZ
| 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 |
3483 |
3471 |
17.78 |
|
|
|
| 2 |
A |
1238 |
1234 |
0.02 |
|
|
|
| 3 |
A |
908 |
905 |
11.66 |
|
|
|
| 4 |
A |
694 |
691 |
83.19 |
|
|
|
| 5 |
A |
524 |
522 |
0.42 |
|
|
|
| 6 |
B |
3481 |
3469 |
105.68 |
|
|
|
| 7 |
B |
2144 |
2136 |
587.89 |
|
|
|
| 8 |
B |
905 |
902 |
418.29 |
|
|
|
| 9 |
B |
528 |
526 |
58.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6951.5 cm
-1
Scaled (by 0.9966) Zero Point Vibrational Energy (zpe) 6927.8 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 BLYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.165 |
|
|
|
| 2 |
N |
-0.212 |
|
|
|
| 3 |
N |
-0.212 |
|
|
|
| 4 |
H |
0.129 |
|
|
|
| 5 |
H |
0.129 |
|
|
|
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 |
1.881 |
1.881 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.319 |
4.020 |
0.000 |
| y |
4.020 |
-16.492 |
0.000 |
| z |
0.000 |
0.000 |
-17.822 |
|
| Traceless |
| | x | y | z |
| x |
-0.162 |
4.020 |
0.000 |
| y |
4.020 |
1.079 |
0.000 |
| z |
0.000 |
0.000 |
-0.916 |
|
| Polar |
| 3z2-r2 | -1.832 |
| x2-y2 | -0.827 |
| xy | 4.020 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.316 |
0.272 |
0.000 |
| y |
0.272 |
7.215 |
0.000 |
| z |
0.000 |
0.000 |
3.288 |
<r2> (average value of r
2) Å
2
| <r2> |
39.527 |
| (<r2>)1/2 |
6.287 |