Vibrational Frequencies calculated at wB97X-D/aug-cc-pVDZ
| 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 |
3631 |
3476 |
24.15 |
|
|
|
| 2 |
A |
1295 |
1240 |
0.00 |
|
|
|
| 3 |
A |
940 |
900 |
10.83 |
|
|
|
| 4 |
A |
738 |
706 |
89.89 |
|
|
|
| 5 |
A |
539 |
516 |
0.11 |
|
|
|
| 6 |
B |
3628 |
3473 |
147.78 |
|
|
|
| 7 |
B |
2235 |
2139 |
739.43 |
|
|
|
| 8 |
B |
941 |
900 |
418.13 |
|
|
|
| 9 |
B |
542 |
519 |
76.37 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7243.8 cm
-1
Scaled (by 0.9573) Zero Point Vibrational Energy (zpe) 6934.5 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/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.101 |
|
|
|
| 2 |
N |
-0.084 |
|
|
|
| 3 |
N |
-0.084 |
|
|
|
| 4 |
H |
0.034 |
|
|
|
| 5 |
H |
0.034 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.032 |
2.032 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.983 |
4.199 |
0.000 |
| y |
4.199 |
-16.760 |
0.000 |
| z |
0.000 |
0.000 |
-17.494 |
|
| Traceless |
| | x | y | z |
| x |
0.144 |
4.199 |
0.000 |
| y |
4.199 |
0.479 |
0.000 |
| z |
0.000 |
0.000 |
-0.622 |
|
| Polar |
| 3z2-r2 | -1.244 |
| x2-y2 | -0.223 |
| xy | 4.199 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.090 |
0.247 |
0.000 |
| y |
0.247 |
6.799 |
0.000 |
| z |
0.000 |
0.000 |
3.062 |
<r2> (average value of r
2) Å
2
| <r2> |
39.106 |
| (<r2>)1/2 |
6.253 |