Vibrational Frequencies calculated at wB97X-D/CEP-31G*
| 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 |
3646 |
3646 |
23.41 |
|
|
|
| 2 |
A |
1293 |
1293 |
0.08 |
|
|
|
| 3 |
A |
949 |
949 |
5.59 |
|
|
|
| 4 |
A |
755 |
755 |
110.82 |
|
|
|
| 5 |
A |
530 |
530 |
0.01 |
|
|
|
| 6 |
B |
3645 |
3645 |
113.60 |
|
|
|
| 7 |
B |
2239 |
2239 |
713.65 |
|
|
|
| 8 |
B |
948 |
948 |
439.34 |
|
|
|
| 9 |
B |
530 |
530 |
92.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7267.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7267.1 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 wB97X-D/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.517 |
|
|
|
| 2 |
N |
-0.068 |
|
|
|
| 3 |
N |
-0.068 |
|
|
|
| 4 |
H |
0.327 |
|
|
|
| 5 |
H |
0.327 |
|
|
|
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 |
2.344 |
2.344 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.534 |
4.627 |
0.000 |
| y |
4.627 |
-16.602 |
0.000 |
| z |
0.000 |
0.000 |
-17.131 |
|
| Traceless |
| | x | y | z |
| x |
0.332 |
4.627 |
0.000 |
| y |
4.627 |
0.230 |
0.000 |
| z |
0.000 |
0.000 |
-0.562 |
|
| Polar |
| 3z2-r2 | -1.125 |
| x2-y2 | 0.068 |
| xy | 4.627 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.169 |
0.289 |
0.000 |
| y |
0.289 |
6.092 |
0.000 |
| z |
0.000 |
0.000 |
2.137 |
<r2> (average value of r
2) Å
2
| <r2> |
33.288 |
| (<r2>)1/2 |
5.770 |