Vibrational Frequencies calculated at PBEPBE/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' |
3349 |
3311 |
3.31 |
|
|
|
| 2 |
A' |
3066 |
3031 |
31.97 |
|
|
|
| 3 |
A' |
2950 |
2916 |
59.59 |
|
|
|
| 4 |
A' |
1666 |
1647 |
23.27 |
|
|
|
| 5 |
A' |
1453 |
1436 |
3.23 |
|
|
|
| 6 |
A' |
1325 |
1310 |
30.12 |
|
|
|
| 7 |
A' |
1036 |
1024 |
35.55 |
|
|
|
| 8 |
A" |
1129 |
1117 |
52.92 |
|
|
|
| 9 |
A" |
1052 |
1040 |
18.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8512.6 cm
-1
Scaled (by 0.9886) Zero Point Vibrational Energy (zpe) 8415.5 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 PBEPBE/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.214 |
|
|
|
| 2 |
N |
-0.331 |
|
|
|
| 3 |
H |
0.135 |
|
|
|
| 4 |
H |
0.155 |
|
|
|
| 5 |
H |
0.255 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.526 |
1.508 |
0.000 |
2.145 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.872 |
2.221 |
0.000 |
| y |
2.221 |
-13.108 |
0.000 |
| z |
0.000 |
0.000 |
-13.909 |
|
| Traceless |
| | x | y | z |
| x |
1.636 |
2.221 |
0.000 |
| y |
2.221 |
-0.217 |
0.000 |
| z |
0.000 |
0.000 |
-1.419 |
|
| Polar |
| 3z2-r2 | -2.839 |
| x2-y2 | 1.235 |
| xy | 2.221 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.940 |
0.080 |
0.000 |
| y |
0.080 |
4.315 |
0.000 |
| z |
0.000 |
0.000 |
1.978 |
<r2> (average value of r
2) Å
2
| <r2> |
20.030 |
| (<r2>)1/2 |
4.475 |