Vibrational Frequencies calculated at B3LYP/LANL2DZ
| 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' |
3396 |
3264 |
15.53 |
|
|
|
| 2 |
A' |
3182 |
3058 |
37.08 |
|
|
|
| 3 |
A' |
3047 |
2929 |
60.56 |
|
|
|
| 4 |
A' |
1669 |
1604 |
8.42 |
|
|
|
| 5 |
A' |
1505 |
1446 |
6.34 |
|
|
|
| 6 |
A' |
1334 |
1282 |
44.37 |
|
|
|
| 7 |
A' |
1075 |
1034 |
53.65 |
|
|
|
| 8 |
A" |
1166 |
1121 |
72.39 |
|
|
|
| 9 |
A" |
1127 |
1083 |
28.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8750.0 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 8410.5 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/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.386 |
|
|
|
| 2 |
N |
-0.243 |
|
|
|
| 3 |
H |
0.189 |
|
|
|
| 4 |
H |
0.211 |
|
|
|
| 5 |
H |
0.229 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.708 |
1.565 |
0.000 |
2.317 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.646 |
2.363 |
0.000 |
| y |
2.363 |
-12.506 |
0.000 |
| z |
0.000 |
0.000 |
-13.658 |
|
| Traceless |
| | x | y | z |
| x |
1.436 |
2.363 |
0.000 |
| y |
2.363 |
0.146 |
0.000 |
| z |
0.000 |
0.000 |
-1.582 |
|
| Polar |
| 3z2-r2 | -3.164 |
| x2-y2 | 0.860 |
| xy | 2.363 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.410 |
0.289 |
0.000 |
| y |
0.289 |
3.726 |
0.000 |
| z |
0.000 |
0.000 |
1.156 |
<r2> (average value of r
2) Å
2
| <r2> |
19.992 |
| (<r2>)1/2 |
4.471 |