Vibrational Frequencies calculated at B3LYP/CEP-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' |
3432 |
3315 |
6.56 |
|
|
|
| 2 |
A' |
3144 |
3037 |
49.49 |
|
|
|
| 3 |
A' |
3034 |
2930 |
67.91 |
|
|
|
| 4 |
A' |
1700 |
1642 |
27.62 |
|
|
|
| 5 |
A' |
1484 |
1433 |
6.50 |
|
|
|
| 6 |
A' |
1374 |
1327 |
37.21 |
|
|
|
| 7 |
A' |
1072 |
1035 |
30.63 |
|
|
|
| 8 |
A" |
1153 |
1114 |
54.88 |
|
|
|
| 9 |
A" |
1083 |
1046 |
20.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8738.8 cm
-1
Scaled (by 0.9657) Zero Point Vibrational Energy (zpe) 8439.1 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 B3LYP/CEP-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.532 |
|
|
|
| 2 |
N |
-0.092 |
|
|
|
| 3 |
H |
0.187 |
|
|
|
| 4 |
H |
0.203 |
|
|
|
| 5 |
H |
0.234 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.507 |
1.586 |
0.000 |
2.188 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.390 |
2.108 |
0.000 |
| y |
2.108 |
-12.509 |
0.000 |
| z |
0.000 |
0.000 |
-13.581 |
|
| Traceless |
| | x | y | z |
| x |
1.655 |
2.108 |
0.000 |
| y |
2.108 |
-0.024 |
0.000 |
| z |
0.000 |
0.000 |
-1.632 |
|
| Polar |
| 3z2-r2 | -3.263 |
| x2-y2 | 1.119 |
| xy | 2.108 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.432 |
0.275 |
-0.000 |
| y |
0.275 |
3.662 |
0.000 |
| z |
-0.000 |
0.000 |
1.506 |
<r2> (average value of r
2) Å
2
| <r2> |
18.121 |
| (<r2>)1/2 |
4.257 |