Vibrational Frequencies calculated at B3LYPultrafine/3-21G
| 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 |
3555 |
3430 |
16.74 |
|
|
|
| 2 |
A |
1298 |
1252 |
0.12 |
|
|
|
| 3 |
A |
804 |
776 |
16.83 |
|
|
|
| 4 |
A |
680 |
656 |
149.03 |
|
|
|
| 5 |
A |
539 |
521 |
1.54 |
|
|
|
| 6 |
B |
3556 |
3431 |
131.00 |
|
|
|
| 7 |
B |
2297 |
2217 |
411.19 |
|
|
|
| 8 |
B |
808 |
780 |
580.32 |
|
|
|
| 9 |
B |
551 |
531 |
78.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7043.9 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 6796.7 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 B3LYPultrafine/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.751 |
|
|
|
| 2 |
N |
-0.686 |
|
|
|
| 3 |
N |
-0.686 |
|
|
|
| 4 |
H |
0.311 |
|
|
|
| 5 |
H |
0.311 |
|
|
|
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 |
2.251 |
2.251 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.479 |
4.529 |
0.000 |
| y |
4.529 |
-14.604 |
0.000 |
| z |
0.000 |
0.000 |
-17.098 |
|
| Traceless |
| | x | y | z |
| x |
-0.628 |
4.529 |
0.000 |
| y |
4.529 |
2.184 |
0.000 |
| z |
0.000 |
0.000 |
-1.556 |
|
| Polar |
| 3z2-r2 | -3.113 |
| x2-y2 | -1.875 |
| xy | 4.529 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.286 |
0.389 |
0.000 |
| y |
0.389 |
5.603 |
0.000 |
| z |
0.000 |
0.000 |
1.230 |
<r2> (average value of r
2) Å
2
| <r2> |
38.995 |
| (<r2>)1/2 |
6.245 |