Vibrational Frequencies calculated at HF/6-31G(2df,p)
| 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 |
3134 |
2838 |
51.87 |
|
|
|
| 2 |
A1 |
1296 |
1174 |
53.14 |
|
|
|
| 3 |
A1 |
599 |
543 |
41.75 |
|
|
|
| 4 |
E |
3199 |
2897 |
21.24 |
|
|
|
| 4 |
E |
3199 |
2897 |
21.24 |
|
|
|
| 5 |
E |
1567 |
1419 |
2.58 |
|
|
|
| 5 |
E |
1567 |
1419 |
2.58 |
|
|
|
| 6 |
E |
656 |
594 |
118.15 |
|
|
|
| 6 |
E |
656 |
594 |
118.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7935.8 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 7185.9 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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cu |
0.413 |
|
|
|
| 2 |
C |
-0.779 |
|
|
|
| 3 |
H |
0.122 |
|
|
|
| 4 |
H |
0.122 |
|
|
|
| 5 |
H |
0.122 |
|
|
|
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 |
3.419 |
3.419 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.273 |
0.000 |
0.000 |
| y |
0.000 |
-20.273 |
0.000 |
| z |
0.000 |
0.000 |
-19.393 |
|
| Traceless |
| | x | y | z |
| x |
-0.440 |
0.000 |
0.000 |
| y |
0.000 |
-0.440 |
0.000 |
| z |
0.000 |
0.000 |
0.879 |
|
| Polar |
| 3z2-r2 | 1.759 |
| 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 |
5.392 |
0.000 |
0.000 |
| y |
0.000 |
5.392 |
0.000 |
| z |
0.000 |
0.000 |
7.660 |
<r2> (average value of r
2) Å
2
| <r2> |
43.606 |
| (<r2>)1/2 |
6.603 |