Vibrational Frequencies calculated at mPW1PW91/6-311+G(3df,2p)
| 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 |
3646 |
3646 |
27.23 |
|
|
|
| 2 |
A |
1307 |
1307 |
0.00 |
|
|
|
| 3 |
A |
910 |
910 |
12.83 |
|
|
|
| 4 |
A |
722 |
722 |
92.93 |
|
|
|
| 5 |
A |
550 |
550 |
0.51 |
|
|
|
| 6 |
B |
3643 |
3643 |
158.46 |
|
|
|
| 7 |
B |
2254 |
2254 |
715.35 |
|
|
|
| 8 |
B |
910 |
910 |
430.70 |
|
|
|
| 9 |
B |
554 |
554 |
83.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7247.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7247.8 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 mPW1PW91/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
1.465 |
|
|
|
| 2 |
N |
-0.932 |
|
|
|
| 3 |
N |
-0.932 |
|
|
|
| 4 |
H |
0.200 |
|
|
|
| 5 |
H |
0.200 |
|
|
|
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 |
1.979 |
1.979 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.964 |
4.147 |
0.000 |
| y |
4.147 |
-16.317 |
0.000 |
| z |
0.000 |
0.000 |
-17.472 |
|
| Traceless |
| | x | y | z |
| x |
-0.069 |
4.147 |
0.000 |
| y |
4.147 |
0.901 |
0.000 |
| z |
0.000 |
0.000 |
-0.831 |
|
| Polar |
| 3z2-r2 | -1.662 |
| x2-y2 | -0.647 |
| xy | 4.147 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.981 |
0.228 |
0.000 |
| y |
0.228 |
6.679 |
0.000 |
| z |
0.000 |
0.000 |
2.953 |
<r2> (average value of r
2) Å
2
| <r2> |
38.685 |
| (<r2>)1/2 |
6.220 |