Vibrational Frequencies calculated at B97D3/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3133 |
3088 |
10.08 |
|
|
|
| 2 |
A1 |
2163 |
2132 |
298.40 |
|
|
|
| 3 |
A1 |
1398 |
1378 |
30.99 |
|
|
|
| 4 |
A1 |
1182 |
1165 |
1.44 |
|
|
|
| 5 |
B1 |
558 |
550 |
4.35 |
|
|
|
| 6 |
B1 |
357 |
352 |
142.25 |
|
|
|
| 7 |
B2 |
3253 |
3207 |
1.01 |
|
|
|
| 8 |
B2 |
1084 |
1068 |
1.02 |
|
|
|
| 9 |
B2 |
414 |
408 |
0.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6771.0 cm
-1
Scaled (by 0.9857) Zero Point Vibrational Energy (zpe) 6674.2 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 B97D3/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.253 |
|
|
|
| 2 |
N |
0.104 |
|
|
|
| 3 |
N |
-0.152 |
|
|
|
| 4 |
H |
0.150 |
|
|
|
| 5 |
H |
0.150 |
|
|
|
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 |
-1.647 |
1.647 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.861 |
0.000 |
0.000 |
| y |
0.000 |
-15.299 |
0.000 |
| z |
0.000 |
0.000 |
-18.504 |
|
| Traceless |
| | x | y | z |
| x |
-1.960 |
0.000 |
0.000 |
| y |
0.000 |
3.383 |
0.000 |
| z |
0.000 |
0.000 |
-1.423 |
|
| Polar |
| 3z2-r2 | -2.847 |
| x2-y2 | -3.562 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.993 |
0.000 |
0.000 |
| y |
0.000 |
2.341 |
0.000 |
| z |
0.000 |
0.000 |
6.733 |
<r2> (average value of r
2) Å
2
| <r2> |
38.118 |
| (<r2>)1/2 |
6.174 |