Vibrational Frequencies calculated at wB97X-D/6-31G*
| 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' |
3479 |
3300 |
3.77 |
|
|
|
| 2 |
A' |
3180 |
3016 |
40.13 |
|
|
|
| 3 |
A' |
3071 |
2913 |
46.07 |
|
|
|
| 4 |
A' |
1761 |
1670 |
26.10 |
|
|
|
| 5 |
A' |
1524 |
1445 |
5.12 |
|
|
|
| 6 |
A' |
1398 |
1326 |
44.66 |
|
|
|
| 7 |
A' |
1097 |
1040 |
37.53 |
|
|
|
| 8 |
A" |
1186 |
1125 |
53.39 |
|
|
|
| 9 |
A" |
1105 |
1049 |
14.90 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8900.0 cm
-1
Scaled (by 0.9485) Zero Point Vibrational Energy (zpe) 8441.7 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*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.150 |
|
|
|
| 2 |
N |
-0.486 |
|
|
|
| 3 |
H |
0.152 |
|
|
|
| 4 |
H |
0.175 |
|
|
|
| 5 |
H |
0.309 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.479 |
1.451 |
0.000 |
2.072 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.382 |
2.040 |
0.000 |
| y |
2.040 |
-12.437 |
0.000 |
| z |
0.000 |
0.000 |
-13.298 |
|
| Traceless |
| | x | y | z |
| x |
1.486 |
2.040 |
0.000 |
| y |
2.040 |
-0.097 |
0.000 |
| z |
0.000 |
0.000 |
-1.389 |
|
| Polar |
| 3z2-r2 | -2.777 |
| x2-y2 | 1.055 |
| xy | 2.040 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.555 |
0.268 |
0.000 |
| y |
0.268 |
3.645 |
0.000 |
| z |
0.000 |
0.000 |
1.162 |
<r2> (average value of r
2) Å
2
| <r2> |
19.429 |
| (<r2>)1/2 |
4.408 |