Vibrational Frequencies calculated at B3LYP/CEP-121G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3451 |
3345 |
74.73 |
|
|
|
| 2 |
Σ |
2321 |
2250 |
28.28 |
|
|
|
| 3 |
Σ |
2135 |
2070 |
0.19 |
|
|
|
| 4 |
Σ |
886 |
859 |
0.00 |
|
|
|
| 5 |
Π |
877 |
851 |
56.82 |
|
|
|
| 5 |
Π |
877 |
851 |
56.82 |
|
|
|
| 6 |
Π |
611 |
593 |
19.64 |
|
|
|
| 6 |
Π |
611 |
593 |
19.64 |
|
|
|
| 7 |
Π |
296 |
287 |
0.04 |
|
|
|
| 7 |
Π |
296 |
287 |
0.04 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6180.3 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 5991.2 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 B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.084 |
|
|
|
| 2 |
C |
-0.555 |
|
|
|
| 3 |
C |
1.175 |
|
|
|
| 4 |
C |
-1.172 |
|
|
|
| 5 |
H |
0.467 |
|
|
|
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 |
-3.880 |
3.880 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.597 |
0.000 |
0.000 |
| y |
0.000 |
-22.597 |
0.000 |
| z |
0.000 |
0.000 |
-20.124 |
|
| Traceless |
| | x | y | z |
| x |
-1.236 |
0.000 |
0.000 |
| y |
0.000 |
-1.236 |
0.000 |
| z |
0.000 |
0.000 |
2.472 |
|
| Polar |
| 3z2-r2 | 4.945 |
| x2-y2 | 0.000 |
| 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 |
2.473 |
0.000 |
0.000 |
| y |
0.000 |
2.473 |
0.000 |
| z |
0.000 |
0.000 |
10.181 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |