Vibrational Frequencies calculated at HF/aug-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 |
3624 |
3300 |
81.57 |
|
|
|
| 2 |
Σ |
2633 |
2397 |
49.97 |
|
|
|
| 3 |
Σ |
2361 |
2150 |
1.04 |
|
|
|
| 4 |
Σ |
932 |
848 |
0.00 |
|
|
|
| 5 |
Π |
803 |
731 |
42.99 |
|
|
|
| 5 |
Π |
803 |
731 |
42.99 |
|
|
|
| 6 |
Π |
587 |
535 |
10.69 |
|
|
|
| 6 |
Π |
587 |
535 |
10.69 |
|
|
|
| 7 |
Π |
252 |
230 |
0.09 |
|
|
|
| 7 |
Π |
252 |
230 |
0.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6416.5 cm
-1
Scaled (by 0.9106) Zero Point Vibrational Energy (zpe) 5842.8 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 HF/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.377 |
|
|
|
| 2 |
C |
-0.348 |
|
|
|
| 3 |
C |
0.633 |
|
|
|
| 4 |
C |
0.571 |
|
|
|
| 5 |
H |
-0.479 |
|
|
|
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 |
-4.105 |
4.105 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.207 |
0.000 |
0.000 |
| y |
0.000 |
-23.207 |
0.000 |
| z |
0.000 |
0.000 |
-21.037 |
|
| Traceless |
| | x | y | z |
| x |
-1.085 |
0.000 |
0.000 |
| y |
0.000 |
-1.085 |
0.000 |
| z |
0.000 |
0.000 |
2.170 |
|
| Polar |
| 3z2-r2 | 4.339 |
| 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 |
3.670 |
0.000 |
0.000 |
| y |
0.000 |
3.670 |
0.000 |
| z |
0.000 |
0.000 |
9.526 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |