Vibrational Frequencies calculated at B3LYPultrafine/6-31+G**
| 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 |
3608 |
3473 |
23.89 |
|
|
|
| 2 |
A |
1288 |
1240 |
0.08 |
|
|
|
| 3 |
A |
891 |
858 |
8.78 |
|
|
|
| 4 |
A |
723 |
696 |
114.71 |
|
|
|
| 5 |
A |
533 |
513 |
0.11 |
|
|
|
| 6 |
B |
3606 |
3471 |
138.66 |
|
|
|
| 7 |
B |
2222 |
2139 |
688.75 |
|
|
|
| 8 |
B |
892 |
858 |
451.49 |
|
|
|
| 9 |
B |
527 |
508 |
75.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7144.5 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 6878.0 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/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.537 |
|
|
|
| 2 |
N |
-0.572 |
|
|
|
| 3 |
N |
-0.572 |
|
|
|
| 4 |
H |
0.304 |
|
|
|
| 5 |
H |
0.304 |
|
|
|
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 |
2.269 |
2.269 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.151 |
4.573 |
0.000 |
| y |
4.573 |
-16.752 |
0.000 |
| z |
0.000 |
0.000 |
-17.729 |
|
| Traceless |
| | x | y | z |
| x |
0.089 |
4.573 |
0.000 |
| y |
4.573 |
0.688 |
0.000 |
| z |
0.000 |
0.000 |
-0.777 |
|
| Polar |
| 3z2-r2 | -1.554 |
| x2-y2 | -0.399 |
| xy | 4.573 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.445 |
0.192 |
0.000 |
| y |
0.192 |
6.837 |
0.000 |
| z |
0.000 |
0.000 |
2.429 |
<r2> (average value of r
2) Å
2
| <r2> |
39.393 |
| (<r2>)1/2 |
6.276 |