Vibrational Frequencies calculated at wB97X-D/6-31G(2df,p)
| 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' |
3496 |
3496 |
0.42 |
|
|
|
| 2 |
A' |
3149 |
3149 |
35.68 |
|
|
|
| 3 |
A' |
3048 |
3048 |
41.53 |
|
|
|
| 4 |
A' |
1748 |
1748 |
23.65 |
|
|
|
| 5 |
A' |
1503 |
1503 |
5.35 |
|
|
|
| 6 |
A' |
1376 |
1376 |
45.49 |
|
|
|
| 7 |
A' |
1083 |
1083 |
37.10 |
|
|
|
| 8 |
A" |
1181 |
1181 |
45.03 |
|
|
|
| 9 |
A" |
1107 |
1107 |
12.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8845.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8845.3 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.181 |
|
|
|
| 2 |
N |
-0.348 |
|
|
|
| 3 |
H |
0.130 |
|
|
|
| 4 |
H |
0.146 |
|
|
|
| 5 |
H |
0.254 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.343 |
1.393 |
0.000 |
1.935 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.330 |
1.916 |
0.000 |
| y |
1.916 |
-12.314 |
0.000 |
| z |
0.000 |
0.000 |
-13.215 |
|
| Traceless |
| | x | y | z |
| x |
1.435 |
1.916 |
0.000 |
| y |
1.916 |
-0.042 |
0.000 |
| z |
0.000 |
0.000 |
-1.393 |
|
| Polar |
| 3z2-r2 | -2.786 |
| x2-y2 | 0.984 |
| xy | 1.916 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.685 |
0.264 |
0.000 |
| y |
0.264 |
3.667 |
0.000 |
| z |
0.000 |
0.000 |
1.526 |
<r2> (average value of r
2) Å
2
| <r2> |
19.337 |
| (<r2>)1/2 |
4.397 |