Vibrational Frequencies calculated at wB97X-D/6-311G**
| 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 |
3648 |
3489 |
29.96 |
|
|
|
| 2 |
A |
1306 |
1249 |
0.11 |
|
|
|
| 3 |
A |
913 |
873 |
10.47 |
|
|
|
| 4 |
A |
741 |
709 |
107.15 |
|
|
|
| 5 |
A |
539 |
515 |
0.15 |
|
|
|
| 6 |
B |
3646 |
3487 |
135.60 |
|
|
|
| 7 |
B |
2267 |
2169 |
665.65 |
|
|
|
| 8 |
B |
914 |
874 |
438.13 |
|
|
|
| 9 |
B |
542 |
518 |
90.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7257.3 cm
-1
Scaled (by 0.9565) Zero Point Vibrational Energy (zpe) 6941.6 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/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.425 |
|
|
|
| 2 |
N |
-0.450 |
|
|
|
| 3 |
N |
-0.450 |
|
|
|
| 4 |
H |
0.237 |
|
|
|
| 5 |
H |
0.237 |
|
|
|
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 |
2.199 |
2.199 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.502 |
4.310 |
0.000 |
| y |
4.310 |
-16.385 |
0.000 |
| z |
0.000 |
0.000 |
-17.059 |
|
| Traceless |
| | x | y | z |
| x |
0.220 |
4.310 |
0.000 |
| y |
4.310 |
0.396 |
0.000 |
| z |
0.000 |
0.000 |
-0.615 |
|
| Polar |
| 3z2-r2 | -1.231 |
| x2-y2 | -0.117 |
| xy | 4.310 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.027 |
0.328 |
0.000 |
| y |
0.328 |
5.931 |
0.000 |
| z |
0.000 |
0.000 |
1.996 |
<r2> (average value of r
2) Å
2
| <r2> |
38.552 |
| (<r2>)1/2 |
6.209 |