Vibrational Frequencies calculated at PBEPBE/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 |
3120 |
3088 |
10.75 |
|
|
|
| 2 |
A1 |
2165 |
2143 |
289.13 |
|
|
|
| 3 |
A1 |
1391 |
1376 |
32.12 |
|
|
|
| 4 |
A1 |
1190 |
1177 |
0.43 |
|
|
|
| 5 |
B1 |
560 |
554 |
2.72 |
|
|
|
| 6 |
B1 |
318 |
315 |
154.82 |
|
|
|
| 7 |
B2 |
3237 |
3204 |
1.37 |
|
|
|
| 8 |
B2 |
1082 |
1071 |
0.54 |
|
|
|
| 9 |
B2 |
418 |
413 |
0.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6740.3 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 6670.2 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 PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.445 |
|
|
|
| 2 |
N |
0.091 |
|
|
|
| 3 |
N |
-0.139 |
|
|
|
| 4 |
H |
0.247 |
|
|
|
| 5 |
H |
0.247 |
|
|
|
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 |
-1.675 |
1.675 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.092 |
0.000 |
0.000 |
| y |
0.000 |
-15.317 |
0.000 |
| z |
0.000 |
0.000 |
-18.556 |
|
| Traceless |
| | x | y | z |
| x |
-2.155 |
0.000 |
0.000 |
| y |
0.000 |
3.507 |
0.000 |
| z |
0.000 |
0.000 |
-1.352 |
|
| Polar |
| 3z2-r2 | -2.703 |
| x2-y2 | -3.775 |
| 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 |
1.963 |
0.000 |
0.000 |
| y |
0.000 |
2.323 |
0.000 |
| z |
0.000 |
0.000 |
6.702 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |