Vibrational Frequencies calculated at B2PLYP/6-31G
| 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' |
3393 |
3393 |
14.85 |
|
|
|
| 2 |
A' |
3211 |
3211 |
36.97 |
|
|
|
| 3 |
A' |
3077 |
3077 |
46.76 |
|
|
|
| 4 |
A' |
1692 |
1692 |
9.80 |
|
|
|
| 5 |
A' |
1526 |
1526 |
4.64 |
|
|
|
| 6 |
A' |
1374 |
1374 |
50.99 |
|
|
|
| 7 |
A' |
1089 |
1089 |
53.90 |
|
|
|
| 8 |
A" |
1183 |
1183 |
64.75 |
|
|
|
| 9 |
A" |
1116 |
1116 |
16.61 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8830.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 8830.7 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 B2PLYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.108 |
|
|
|
| 2 |
N |
-0.433 |
|
|
|
| 3 |
H |
0.125 |
|
|
|
| 4 |
H |
0.153 |
|
|
|
| 5 |
H |
0.264 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.658 |
1.438 |
0.000 |
2.195 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.861 |
2.325 |
0.000 |
| y |
2.325 |
-12.763 |
0.000 |
| z |
0.000 |
0.000 |
-13.444 |
|
| Traceless |
| | x | y | z |
| x |
1.242 |
2.325 |
0.000 |
| y |
2.325 |
-0.110 |
0.000 |
| z |
0.000 |
0.000 |
-1.132 |
|
| Polar |
| 3z2-r2 | -2.263 |
| x2-y2 | 0.902 |
| xy | 2.325 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.481 |
0.285 |
0.000 |
| y |
0.285 |
3.722 |
0.000 |
| z |
0.000 |
0.000 |
1.016 |
<r2> (average value of r
2) Å
2
| <r2> |
19.945 |
| (<r2>)1/2 |
4.466 |