Vibrational Frequencies calculated at BLYP/TZVP
| 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 |
3486 |
3477 |
17.97 |
|
|
|
| 2 |
A |
1244 |
1241 |
0.00 |
|
|
|
| 3 |
A |
867 |
865 |
9.05 |
|
|
|
| 4 |
A |
691 |
690 |
107.54 |
|
|
|
| 5 |
A |
519 |
518 |
0.35 |
|
|
|
| 6 |
B |
3485 |
3476 |
100.32 |
|
|
|
| 7 |
B |
2162 |
2157 |
543.87 |
|
|
|
| 8 |
B |
867 |
865 |
429.60 |
|
|
|
| 9 |
B |
521 |
520 |
68.29 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6921.4 cm
-1
Scaled (by 0.9975) Zero Point Vibrational Energy (zpe) 6904.1 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/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.235 |
|
|
|
| 2 |
N |
-0.345 |
|
|
|
| 3 |
N |
-0.345 |
|
|
|
| 4 |
H |
0.227 |
|
|
|
| 5 |
H |
0.227 |
|
|
|
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 |
2.145 |
2.145 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.133 |
4.378 |
0.000 |
| y |
4.378 |
-16.380 |
0.000 |
| z |
0.000 |
0.000 |
-17.707 |
|
| Traceless |
| | x | y | z |
| x |
-0.089 |
4.378 |
0.000 |
| y |
4.378 |
1.040 |
0.000 |
| z |
0.000 |
0.000 |
-0.950 |
|
| Polar |
| 3z2-r2 | -1.901 |
| x2-y2 | -0.753 |
| xy | 4.378 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.363 |
0.292 |
0.000 |
| y |
0.292 |
6.755 |
0.000 |
| z |
0.000 |
0.000 |
2.343 |
<r2> (average value of r
2) Å
2
| <r2> |
39.506 |
| (<r2>)1/2 |
6.285 |