Vibrational Frequencies calculated at B3LYPultrafine/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' |
3254 |
3140 |
20.10 |
|
|
|
| 2 |
A' |
3130 |
3020 |
37.55 |
|
|
|
| 3 |
A' |
3016 |
2910 |
48.78 |
|
|
|
| 4 |
A' |
1697 |
1637 |
7.76 |
|
|
|
| 5 |
A' |
1532 |
1478 |
2.40 |
|
|
|
| 6 |
A' |
1370 |
1322 |
65.57 |
|
|
|
| 7 |
A' |
1098 |
1060 |
48.67 |
|
|
|
| 8 |
A" |
1185 |
1143 |
51.89 |
|
|
|
| 9 |
A" |
1111 |
1072 |
21.73 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8695.5 cm
-1
Scaled (by 0.9649) Zero Point Vibrational Energy (zpe) 8390.3 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 B3LYPultrafine/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 |
| |
-1.516 |
1.231 |
0.000 |
1.953 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.574 |
2.120 |
0.000 |
| y |
2.120 |
-12.501 |
0.000 |
| z |
0.000 |
0.000 |
-13.283 |
|
| Traceless |
| | x | y | z |
| x |
1.318 |
2.120 |
0.000 |
| y |
2.120 |
-0.072 |
0.000 |
| z |
0.000 |
0.000 |
-1.246 |
|
| Polar |
| 3z2-r2 | -2.491 |
| x2-y2 | 0.927 |
| xy | 2.120 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.349 |
0.344 |
0.000 |
| y |
0.344 |
3.456 |
0.000 |
| z |
0.000 |
0.000 |
0.886 |
<r2> (average value of r
2) Å
2
| <r2> |
19.700 |
| (<r2>)1/2 |
4.438 |