Vibrational Frequencies calculated at wB97X-D/LANL2DZ
| 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 |
3479 |
12.38 |
|
|
|
| 2 |
A' |
3221 |
3221 |
37.58 |
|
|
|
| 3 |
A' |
3083 |
3083 |
58.33 |
|
|
|
| 4 |
A' |
1702 |
1702 |
10.42 |
|
|
|
| 5 |
A' |
1521 |
1521 |
7.72 |
|
|
|
| 6 |
A' |
1350 |
1350 |
45.15 |
|
|
|
| 7 |
A' |
1089 |
1089 |
55.17 |
|
|
|
| 8 |
A" |
1181 |
1181 |
71.90 |
|
|
|
| 9 |
A" |
1141 |
1141 |
32.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8882.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8882.1 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/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.368 |
|
|
|
| 2 |
N |
-0.277 |
|
|
|
| 3 |
H |
0.187 |
|
|
|
| 4 |
H |
0.213 |
|
|
|
| 5 |
H |
0.244 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.768 |
1.611 |
0.000 |
2.391 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.552 |
2.419 |
0.000 |
| y |
2.419 |
-12.447 |
0.000 |
| z |
0.000 |
0.000 |
-13.615 |
|
| Traceless |
| | x | y | z |
| x |
1.479 |
2.419 |
0.000 |
| y |
2.419 |
0.137 |
0.000 |
| z |
0.000 |
0.000 |
-1.616 |
|
| Polar |
| 3z2-r2 | -3.231 |
| x2-y2 | 0.894 |
| xy | 2.419 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.385 |
0.278 |
0.000 |
| y |
0.278 |
3.729 |
0.000 |
| z |
0.000 |
0.000 |
1.149 |
<r2> (average value of r
2) Å
2
| <r2> |
19.864 |
| (<r2>)1/2 |
4.457 |