Vibrational Frequencies calculated at PBE1PBE/6-311+G(3df,2p)
| 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' |
3487 |
3487 |
0.54 |
|
|
|
| 2 |
A' |
3132 |
3132 |
27.12 |
|
|
|
| 3 |
A' |
3035 |
3035 |
46.85 |
|
|
|
| 4 |
A' |
1734 |
1734 |
23.53 |
|
|
|
| 5 |
A' |
1489 |
1489 |
7.41 |
|
|
|
| 6 |
A' |
1364 |
1364 |
39.32 |
|
|
|
| 7 |
A' |
1068 |
1068 |
36.45 |
|
|
|
| 8 |
A" |
1169 |
1169 |
44.70 |
|
|
|
| 9 |
A" |
1104 |
1104 |
18.64 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8791.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8791.1 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 PBE1PBE/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.290 |
|
|
|
| 2 |
N |
-0.698 |
|
|
|
| 3 |
H |
0.126 |
|
|
|
| 4 |
H |
0.129 |
|
|
|
| 5 |
H |
0.154 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.379 |
1.496 |
0.000 |
2.035 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.700 |
2.079 |
0.000 |
| y |
2.079 |
-12.763 |
0.000 |
| z |
0.000 |
0.000 |
-13.729 |
|
| Traceless |
| | x | y | z |
| x |
1.547 |
2.079 |
0.000 |
| y |
2.079 |
-0.049 |
0.000 |
| z |
0.000 |
0.000 |
-1.498 |
|
| Polar |
| 3z2-r2 | -2.996 |
| x2-y2 | 1.064 |
| xy | 2.079 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.117 |
0.117 |
0.000 |
| y |
0.117 |
4.233 |
0.000 |
| z |
0.000 |
0.000 |
2.412 |
<r2> (average value of r
2) Å
2
| <r2> |
19.564 |
| (<r2>)1/2 |
4.423 |