Vibrational Frequencies calculated at B3PW91/cc-pVDZ
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3483 |
3361 |
91.15 |
|
|
|
| 2 |
Σ |
2392 |
2309 |
23.52 |
|
|
|
| 3 |
Σ |
2181 |
2105 |
0.50 |
|
|
|
| 4 |
Σ |
916 |
884 |
0.02 |
|
|
|
| 5 |
Π |
703 |
679 |
35.88 |
|
|
|
| 5 |
Π |
703 |
679 |
35.88 |
|
|
|
| 6 |
Π |
554 |
535 |
4.50 |
|
|
|
| 6 |
Π |
554 |
535 |
4.50 |
|
|
|
| 7 |
Π |
245 |
237 |
0.11 |
|
|
|
| 7 |
Π |
245 |
237 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5988.6 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 5779.0 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.097 |
|
|
|
| 2 |
C |
-0.239 |
|
|
|
| 3 |
C |
0.596 |
|
|
|
| 4 |
C |
-0.299 |
|
|
|
| 5 |
H |
0.039 |
|
|
|
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 |
-3.692 |
3.692 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.389 |
0.000 |
0.000 |
| y |
0.000 |
-22.389 |
0.000 |
| z |
0.000 |
0.000 |
-19.925 |
|
| Traceless |
| | x | y | z |
| x |
-1.232 |
0.000 |
0.000 |
| y |
0.000 |
-1.232 |
0.000 |
| z |
0.000 |
0.000 |
2.463 |
|
| Polar |
| 3z2-r2 | 4.926 |
| x2-y2 | 0.000 |
| 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 |
2.274 |
0.000 |
0.000 |
| y |
0.000 |
2.274 |
0.000 |
| z |
0.000 |
0.000 |
9.648 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |