Vibrational Frequencies calculated at B3LYP/3-21G*
| 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' |
3258 |
3134 |
19.56 |
|
|
|
| 2 |
A' |
3127 |
3008 |
38.26 |
|
|
|
| 3 |
A' |
3013 |
2898 |
49.24 |
|
|
|
| 4 |
A' |
1699 |
1635 |
8.00 |
|
|
|
| 5 |
A' |
1533 |
1475 |
2.52 |
|
|
|
| 6 |
A' |
1368 |
1316 |
65.26 |
|
|
|
| 7 |
A' |
1097 |
1055 |
49.55 |
|
|
|
| 8 |
A" |
1183 |
1138 |
51.88 |
|
|
|
| 9 |
A" |
1113 |
1070 |
21.66 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8694.9 cm
-1
Scaled (by 0.962) Zero Point Vibrational Energy (zpe) 8364.5 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 B3LYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
N |
-0.481 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.199 |
|
|
|
| 5 |
H |
0.257 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.517 |
1.228 |
0.000 |
1.951 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.579 |
2.123 |
0.000 |
| y |
2.123 |
-12.495 |
0.000 |
| z |
0.000 |
0.000 |
-13.281 |
|
| Traceless |
| | x | y | z |
| x |
1.309 |
2.123 |
0.000 |
| y |
2.123 |
-0.064 |
0.000 |
| z |
0.000 |
0.000 |
-1.244 |
|
| Polar |
| 3z2-r2 | -2.489 |
| x2-y2 | 0.915 |
| xy | 2.123 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.351 |
0.344 |
0.000 |
| y |
0.344 |
3.462 |
0.000 |
| z |
0.000 |
0.000 |
0.886 |
<r2> (average value of r
2) Å
2
| <r2> |
19.697 |
| (<r2>)1/2 |
4.438 |