Vibrational Frequencies calculated at HF/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 |
3269 |
2970 |
10.18 |
|
|
|
| 2 |
A1 |
1994 |
1811 |
48.04 |
|
|
|
| 3 |
A1 |
1633 |
1483 |
3.50 |
|
|
|
| 4 |
A1 |
1158 |
1052 |
6.32 |
|
|
|
| 5 |
A2 |
1088 |
988 |
0.00 |
|
|
|
| 6 |
B1 |
3380 |
3071 |
25.18 |
|
|
|
| 7 |
B1 |
1248 |
1134 |
6.59 |
|
|
|
| 8 |
B2 |
1162 |
1056 |
26.46 |
|
|
|
| 9 |
B2 |
973 |
884 |
32.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7952.2 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 7224.6 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 HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.089 |
|
|
|
| 2 |
N |
-0.076 |
|
|
|
| 3 |
N |
-0.076 |
|
|
|
| 4 |
H |
0.121 |
|
|
|
| 5 |
H |
0.121 |
|
|
|
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 |
1.840 |
1.840 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.866 |
0.000 |
0.000 |
| y |
0.000 |
-19.887 |
0.000 |
| z |
0.000 |
0.000 |
-17.183 |
|
| Traceless |
| | x | y | z |
| x |
2.669 |
0.000 |
0.000 |
| y |
0.000 |
-3.363 |
0.000 |
| z |
0.000 |
0.000 |
0.694 |
|
| Polar |
| 3z2-r2 | 1.387 |
| x2-y2 | 4.022 |
| 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 |
2.276 |
0.000 |
0.000 |
| y |
0.000 |
2.709 |
0.000 |
| z |
0.000 |
0.000 |
3.919 |
<r2> (average value of r
2) Å
2
| <r2> |
28.933 |
| (<r2>)1/2 |
5.379 |