Vibrational Frequencies calculated at B3LYP/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' |
3365 |
3237 |
17.00 |
|
|
|
| 2 |
A' |
3174 |
3053 |
39.46 |
|
|
|
| 3 |
A' |
3044 |
2928 |
49.58 |
|
|
|
| 4 |
A' |
1710 |
1645 |
15.08 |
|
|
|
| 5 |
A' |
1529 |
1471 |
5.84 |
|
|
|
| 6 |
A' |
1360 |
1309 |
50.69 |
|
|
|
| 7 |
A' |
1081 |
1040 |
53.62 |
|
|
|
| 8 |
A" |
1177 |
1133 |
61.85 |
|
|
|
| 9 |
A" |
1115 |
1073 |
19.16 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8777.1 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 8443.6 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 B3LYP/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.112 |
|
|
|
| 2 |
N |
-0.422 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.151 |
|
|
|
| 5 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.636 |
1.398 |
0.000 |
2.152 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.739 |
2.299 |
0.000 |
| y |
2.299 |
-12.648 |
0.000 |
| z |
0.000 |
0.000 |
-13.345 |
|
| Traceless |
| | x | y | z |
| x |
1.257 |
2.299 |
0.000 |
| y |
2.299 |
-0.105 |
0.000 |
| z |
0.000 |
0.000 |
-1.152 |
|
| Polar |
| 3z2-r2 | -2.303 |
| x2-y2 | 0.908 |
| xy | 2.299 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.506 |
0.293 |
0.000 |
| y |
0.293 |
3.780 |
0.000 |
| z |
0.000 |
0.000 |
1.027 |
<r2> (average value of r
2) Å
2
| <r2> |
19.812 |
| (<r2>)1/2 |
4.451 |