Vibrational Frequencies calculated at wB97X-D/cc-pVTZ
| 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 |
3215 |
3074 |
14.53 |
|
|
|
| 2 |
A1 |
2244 |
2146 |
477.71 |
|
|
|
| 3 |
A1 |
1470 |
1405 |
39.82 |
|
|
|
| 4 |
A1 |
1232 |
1178 |
5.74 |
|
|
|
| 5 |
B1 |
599 |
572 |
2.00 |
|
|
|
| 6 |
B1 |
450 |
430 |
145.50 |
|
|
|
| 7 |
B2 |
3345 |
3198 |
2.41 |
|
|
|
| 8 |
B2 |
1144 |
1094 |
1.73 |
|
|
|
| 9 |
B2 |
442 |
423 |
0.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7070.3 cm
-1
Scaled (by 0.956) Zero Point Vibrational Energy (zpe) 6759.2 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/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.300 |
|
|
|
| 2 |
N |
0.181 |
|
|
|
| 3 |
N |
-0.110 |
|
|
|
| 4 |
H |
0.115 |
|
|
|
| 5 |
H |
0.115 |
|
|
|
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 |
-1.523 |
1.523 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.964 |
0.000 |
0.000 |
| y |
0.000 |
-15.377 |
0.000 |
| z |
0.000 |
0.000 |
-18.594 |
|
| Traceless |
| | x | y | z |
| x |
-1.978 |
0.000 |
0.000 |
| y |
0.000 |
3.402 |
0.000 |
| z |
0.000 |
0.000 |
-1.424 |
|
| Polar |
| 3z2-r2 | -2.847 |
| x2-y2 | -3.587 |
| 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 |
2.354 |
0.000 |
0.000 |
| y |
0.000 |
2.624 |
0.000 |
| z |
0.000 |
0.000 |
6.970 |
<r2> (average value of r
2) Å
2
| <r2> |
37.548 |
| (<r2>)1/2 |
6.128 |