Vibrational Frequencies calculated at PBE1PBE/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' |
3463 |
3300 |
3.74 |
|
|
|
| 2 |
A' |
3175 |
3026 |
38.67 |
|
|
|
| 3 |
A' |
3069 |
2925 |
46.80 |
|
|
|
| 4 |
A' |
1760 |
1678 |
25.75 |
|
|
|
| 5 |
A' |
1518 |
1447 |
4.48 |
|
|
|
| 6 |
A' |
1391 |
1326 |
43.74 |
|
|
|
| 7 |
A' |
1085 |
1034 |
37.44 |
|
|
|
| 8 |
A" |
1185 |
1129 |
52.77 |
|
|
|
| 9 |
A" |
1099 |
1047 |
14.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8871.7 cm
-1
Scaled (by 0.9531) Zero Point Vibrational Energy (zpe) 8455.6 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/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.158 |
|
|
|
| 2 |
N |
-0.485 |
|
|
|
| 3 |
H |
0.155 |
|
|
|
| 4 |
H |
0.178 |
|
|
|
| 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 |
| |
-1.454 |
1.404 |
0.000 |
2.021 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.429 |
2.018 |
0.000 |
| y |
2.018 |
-12.472 |
0.000 |
| z |
0.000 |
0.000 |
-13.327 |
|
| Traceless |
| | x | y | z |
| x |
1.471 |
2.018 |
0.000 |
| y |
2.018 |
-0.094 |
0.000 |
| z |
0.000 |
0.000 |
-1.376 |
|
| Polar |
| 3z2-r2 | -2.753 |
| x2-y2 | 1.043 |
| xy | 2.018 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.563 |
0.262 |
0.000 |
| y |
0.262 |
3.644 |
0.000 |
| z |
0.000 |
0.000 |
1.165 |
<r2> (average value of r
2) Å
2
| <r2> |
19.455 |
| (<r2>)1/2 |
4.411 |