Vibrational Frequencies calculated at wB97X-D/CEP-121G
| 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 |
3700 |
3700 |
11.43 |
|
|
|
| 2 |
A |
1272 |
1272 |
0.04 |
|
|
|
| 3 |
A |
718 |
718 |
14.12 |
|
|
|
| 4 |
A |
649 |
649 |
225.89 |
|
|
|
| 5 |
A |
538 |
538 |
0.65 |
|
|
|
| 6 |
B |
3702 |
3702 |
232.15 |
|
|
|
| 7 |
B |
2229 |
2229 |
703.16 |
|
|
|
| 8 |
B |
719 |
719 |
666.93 |
|
|
|
| 9 |
B |
542 |
542 |
109.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7033.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7033.9 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 wB97X-D/CEP-121G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.295 |
|
|
|
| 2 |
N |
-0.175 |
|
|
|
| 3 |
N |
-0.175 |
|
|
|
| 4 |
H |
0.322 |
|
|
|
| 5 |
H |
0.322 |
|
|
|
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 |
2.463 |
2.463 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.185 |
5.135 |
0.000 |
| y |
5.135 |
-14.434 |
0.000 |
| z |
0.000 |
0.000 |
-17.867 |
|
| Traceless |
| | x | y | z |
| x |
-1.035 |
5.135 |
0.000 |
| y |
5.135 |
3.092 |
0.000 |
| z |
0.000 |
0.000 |
-2.057 |
|
| Polar |
| 3z2-r2 | -4.115 |
| x2-y2 | -2.751 |
| xy | 5.135 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.870 |
0.173 |
0.000 |
| y |
0.173 |
6.593 |
0.000 |
| z |
0.000 |
0.000 |
1.842 |
<r2> (average value of r
2) Å
2
| <r2> |
33.790 |
| (<r2>)1/2 |
5.813 |