Vibrational Frequencies calculated at wB97X-D/STO-3G
| 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' |
3518 |
3518 |
15.24 |
|
|
|
| 2 |
A' |
3490 |
3490 |
4.64 |
|
|
|
| 3 |
A' |
3340 |
3340 |
0.99 |
|
|
|
| 4 |
A' |
1794 |
1794 |
4.66 |
|
|
|
| 5 |
A' |
1574 |
1574 |
0.06 |
|
|
|
| 6 |
A' |
1491 |
1491 |
30.84 |
|
|
|
| 7 |
A' |
1124 |
1124 |
18.51 |
|
|
|
| 8 |
A" |
1241 |
1241 |
23.86 |
|
|
|
| 9 |
A" |
1081 |
1081 |
12.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9326.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 9326.2 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/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.055 |
|
|
|
| 2 |
N |
-0.264 |
|
|
|
| 3 |
H |
0.075 |
|
|
|
| 4 |
H |
0.087 |
|
|
|
| 5 |
H |
0.156 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.352 |
1.209 |
0.000 |
1.813 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-10.702 |
1.540 |
0.000 |
| y |
1.540 |
-12.181 |
0.000 |
| z |
0.000 |
0.000 |
-12.089 |
|
| Traceless |
| | x | y | z |
| x |
1.433 |
1.540 |
0.000 |
| y |
1.540 |
-0.786 |
0.000 |
| z |
0.000 |
0.000 |
-0.648 |
|
| Polar |
| 3z2-r2 | -1.295 |
| x2-y2 | 1.479 |
| xy | 1.540 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.419 |
0.377 |
0.000 |
| y |
0.377 |
2.135 |
0.000 |
| z |
0.000 |
0.000 |
0.448 |
<r2> (average value of r
2) Å
2
| <r2> |
19.516 |
| (<r2>)1/2 |
4.418 |