Vibrational Frequencies calculated at B3LYP/LANL2DZ
| 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 |
3038 |
2920 |
29.71 |
|
|
|
| 2 |
A1 |
1153 |
1108 |
16.90 |
|
|
|
| 3 |
A1 |
539 |
518 |
2.18 |
|
|
|
| 4 |
E |
3159 |
3037 |
12.04 |
|
|
|
| 4 |
E |
3159 |
3037 |
12.03 |
|
|
|
| 5 |
E |
1469 |
1412 |
1.17 |
|
|
|
| 5 |
E |
1469 |
1412 |
1.17 |
|
|
|
| 6 |
E |
693 |
666 |
76.09 |
|
|
|
| 6 |
E |
693 |
666 |
76.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7685.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 7387.3 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 B3LYP/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cu |
0.202 |
|
|
|
| 2 |
C |
-0.871 |
|
|
|
| 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 |
1.650 |
1.650 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.646 |
0.000 |
0.000 |
| y |
0.000 |
-20.646 |
0.000 |
| z |
0.000 |
0.000 |
-19.193 |
|
| Traceless |
| | x | y | z |
| x |
-0.726 |
0.000 |
0.000 |
| y |
0.000 |
-0.726 |
0.000 |
| z |
0.000 |
0.000 |
1.453 |
|
| Polar |
| 3z2-r2 | 2.905 |
| 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 |
5.390 |
0.000 |
0.000 |
| y |
0.000 |
5.391 |
-0.001 |
| z |
0.000 |
-0.001 |
8.628 |
<r2> (average value of r
2) Å
2
| <r2> |
42.286 |
| (<r2>)1/2 |
6.503 |