Vibrational Frequencies calculated at PBEPBE/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 |
2944 |
2913 |
40.54 |
|
|
|
| 2 |
A1 |
1192 |
1180 |
42.59 |
|
|
|
| 3 |
A1 |
592 |
586 |
1.49 |
|
|
|
| 4 |
E |
3029 |
2998 |
29.07 |
|
|
|
| 4 |
E |
3029 |
2998 |
29.07 |
|
|
|
| 5 |
E |
1408 |
1393 |
1.64 |
|
|
|
| 5 |
E |
1408 |
1393 |
1.64 |
|
|
|
| 6 |
E |
706 |
698 |
41.42 |
|
|
|
| 6 |
E |
706 |
698 |
41.42 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7506.3 cm
-1
Scaled (by 0.9896) Zero Point Vibrational Energy (zpe) 7428.2 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 PBEPBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cu |
0.307 |
|
|
|
| 2 |
C |
-0.976 |
|
|
|
| 3 |
H |
0.223 |
|
|
|
| 4 |
H |
0.223 |
|
|
|
| 5 |
H |
0.223 |
|
|
|
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 |
1.628 |
1.628 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.475 |
0.000 |
0.000 |
| y |
0.000 |
-21.475 |
0.000 |
| z |
0.000 |
0.000 |
-20.288 |
|
| Traceless |
| | x | y | z |
| x |
-0.594 |
0.000 |
0.000 |
| y |
0.000 |
-0.594 |
0.000 |
| z |
0.000 |
0.000 |
1.187 |
|
| Polar |
| 3z2-r2 | 2.374 |
| 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 |
2.761 |
0.000 |
0.000 |
| y |
0.000 |
2.761 |
0.000 |
| z |
0.000 |
0.000 |
8.254 |
<r2> (average value of r
2) Å
2
| <r2> |
43.467 |
| (<r2>)1/2 |
6.593 |