Vibrational Frequencies calculated at M06-2X/daug-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 |
A |
3619 |
3619 |
32.82 |
|
|
|
| 2 |
A |
1313 |
1313 |
0.01 |
|
|
|
| 3 |
A |
913 |
913 |
12.56 |
|
|
|
| 4 |
A |
735 |
735 |
93.75 |
|
|
|
| 5 |
A |
549 |
549 |
0.67 |
|
|
|
| 6 |
B |
3614 |
3614 |
202.15 |
|
|
|
| 7 |
B |
2247 |
2247 |
806.03 |
|
|
|
| 8 |
B |
911 |
911 |
432.24 |
|
|
|
| 9 |
B |
555 |
555 |
93.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7227.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7227.6 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 M06-2X/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.514 |
|
|
|
| 2 |
N |
-0.816 |
|
|
|
| 3 |
N |
-0.816 |
|
|
|
| 4 |
H |
0.559 |
|
|
|
| 5 |
H |
0.559 |
|
|
|
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 |
2.004 |
2.004 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.045 |
4.174 |
0.000 |
| y |
4.174 |
-16.619 |
0.000 |
| z |
0.000 |
0.000 |
-17.560 |
|
| Traceless |
| | x | y | z |
| x |
0.045 |
4.174 |
0.000 |
| y |
4.174 |
0.683 |
0.000 |
| z |
0.000 |
0.000 |
-0.728 |
|
| Polar |
| 3z2-r2 | -1.456 |
| x2-y2 | -0.426 |
| xy | 4.174 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.091 |
0.259 |
0.000 |
| y |
0.259 |
6.701 |
0.000 |
| z |
0.000 |
0.000 |
3.060 |
<r2> (average value of r
2) Å
2
| <r2> |
38.754 |
| (<r2>)1/2 |
6.225 |