Vibrational Frequencies calculated at wB97X-D/3-21G
| 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' |
3354 |
3354 |
8.63 |
|
|
|
| 2 |
A' |
3172 |
3172 |
36.73 |
|
|
|
| 3 |
A' |
3055 |
3055 |
38.50 |
|
|
|
| 4 |
A' |
1717 |
1717 |
7.93 |
|
|
|
| 5 |
A' |
1541 |
1541 |
3.39 |
|
|
|
| 6 |
A' |
1380 |
1380 |
66.43 |
|
|
|
| 7 |
A' |
1111 |
1111 |
52.26 |
|
|
|
| 8 |
A" |
1198 |
1198 |
57.20 |
|
|
|
| 9 |
A" |
1126 |
1126 |
28.99 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8826.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8826.8 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/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.177 |
|
|
|
| 2 |
N |
-0.507 |
|
|
|
| 3 |
H |
0.186 |
|
|
|
| 4 |
H |
0.221 |
|
|
|
| 5 |
H |
0.277 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.604 |
1.309 |
0.000 |
2.070 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.428 |
2.218 |
0.000 |
| y |
2.218 |
-12.371 |
0.000 |
| z |
0.000 |
0.000 |
-13.310 |
|
| Traceless |
| | x | y | z |
| x |
1.412 |
2.218 |
0.000 |
| y |
2.218 |
-0.002 |
0.000 |
| z |
0.000 |
0.000 |
-1.410 |
|
| Polar |
| 3z2-r2 | -2.821 |
| x2-y2 | 0.942 |
| xy | 2.218 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.300 |
0.326 |
0.000 |
| y |
0.326 |
3.423 |
0.000 |
| z |
0.000 |
0.000 |
0.882 |
<r2> (average value of r
2) Å
2
| <r2> |
19.593 |
| (<r2>)1/2 |
4.426 |