Vibrational Frequencies calculated at B3PW91/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A1 |
3136 |
3019 |
8.73 |
|
|
|
| 2 |
A1 |
1760 |
1694 |
23.13 |
|
|
|
| 3 |
A1 |
1510 |
1453 |
3.25 |
|
|
|
| 4 |
A1 |
1078 |
1038 |
2.71 |
|
|
|
| 5 |
A2 |
1000 |
963 |
0.00 |
|
|
|
| 6 |
B1 |
3253 |
3132 |
18.96 |
|
|
|
| 7 |
B1 |
1162 |
1119 |
4.16 |
|
|
|
| 8 |
B2 |
1010 |
972 |
33.64 |
|
|
|
| 9 |
B2 |
859 |
827 |
25.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7383.4 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 7108.0 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 B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.396 |
|
|
|
| 2 |
N |
-0.042 |
|
|
|
| 3 |
N |
-0.042 |
|
|
|
| 4 |
H |
0.240 |
|
|
|
| 5 |
H |
0.240 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
1.681 |
1.681 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.696 |
0.000 |
0.000 |
| y |
0.000 |
-19.844 |
0.000 |
| z |
0.000 |
0.000 |
-16.994 |
|
| Traceless |
| | x | y | z |
| x |
2.723 |
0.000 |
0.000 |
| y |
0.000 |
-3.500 |
0.000 |
| z |
0.000 |
0.000 |
0.776 |
|
| Polar |
| 3z2-r2 | 1.553 |
| x2-y2 | 4.149 |
| xy | 0.000 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.379 |
0.000 |
0.000 |
| y |
0.000 |
2.733 |
0.000 |
| z |
0.000 |
0.000 |
3.973 |
<r2> (average value of r
2) Å
2
| <r2> |
29.424 |
| (<r2>)1/2 |
5.424 |