Vibrational Frequencies calculated at BLYP/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" |
1052 |
1044 |
10.57 |
|
|
|
| 2 |
A' |
1050 |
1042 |
34.20 |
|
|
|
| 3 |
A' |
3289 |
3264 |
13.33 |
|
|
|
| 4 |
A' |
3039 |
3015 |
44.45 |
|
|
|
| 5 |
A' |
2932 |
2909 |
59.43 |
|
|
|
| 6 |
A' |
1664 |
1651 |
20.39 |
|
|
|
| 7 |
A' |
1468 |
1456 |
3.06 |
|
|
|
| 8 |
A' |
1345 |
1335 |
42.17 |
|
|
|
| 9 |
A" |
1138 |
1130 |
43.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8487.9 cm
-1
Scaled (by 0.9923) Zero Point Vibrational Energy (zpe) 8422.6 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 BLYP/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.003 |
|
|
|
| 2 |
N |
-0.395 |
|
|
|
| 3 |
H |
0.079 |
|
|
|
| 4 |
H |
0.101 |
|
|
|
| 5 |
H |
0.218 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.330 |
1.279 |
0.000 |
1.845 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.617 |
1.892 |
0.000 |
| y |
1.892 |
-12.628 |
0.000 |
| z |
0.000 |
0.000 |
-13.238 |
|
| Traceless |
| | x | y | z |
| x |
1.315 |
1.892 |
0.000 |
| y |
1.892 |
-0.200 |
0.000 |
| z |
0.000 |
0.000 |
-1.115 |
|
| Polar |
| 3z2-r2 | -2.230 |
| x2-y2 | 1.010 |
| xy | 1.892 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.729 |
0.292 |
0.000 |
| y |
0.292 |
3.752 |
0.000 |
| z |
0.000 |
0.000 |
1.216 |
<r2> (average value of r
2) Å
2
| <r2> |
19.755 |
| (<r2>)1/2 |
4.445 |