Vibrational Frequencies calculated at B1B95/6-31G*
| 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 |
3062 |
2907 |
13.69 |
|
|
|
| 2 |
A1 |
1205 |
1144 |
4.42 |
|
|
|
| 3 |
A1 |
527 |
501 |
10.73 |
|
|
|
| 4 |
E |
3156 |
2996 |
10.59 |
|
|
|
| 4 |
E |
3156 |
2996 |
10.60 |
|
|
|
| 5 |
E |
1456 |
1382 |
5.09 |
|
|
|
| 5 |
E |
1456 |
1382 |
5.09 |
|
|
|
| 6 |
E |
616 |
585 |
2.41 |
|
|
|
| 6 |
E |
616 |
585 |
2.40 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7625.8 cm
-1
Scaled (by 0.9493) Zero Point Vibrational Energy (zpe) 7239.1 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 B1B95/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.279 |
|
|
|
| 2 |
C |
-0.816 |
|
|
|
| 3 |
H |
0.179 |
|
|
|
| 4 |
H |
0.179 |
|
|
|
| 5 |
H |
0.179 |
|
|
|
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 |
-0.321 |
0.321 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.315 |
0.000 |
0.000 |
| y |
0.000 |
-21.315 |
0.000 |
| z |
0.000 |
0.000 |
-25.323 |
|
| Traceless |
| | x | y | z |
| x |
2.004 |
0.000 |
0.000 |
| y |
0.000 |
2.004 |
0.000 |
| z |
0.000 |
0.000 |
-4.008 |
|
| Polar |
| 3z2-r2 | -8.016 |
| 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 |
7.052 |
0.000 |
0.000 |
| y |
0.000 |
7.054 |
-0.001 |
| z |
0.000 |
-0.001 |
8.587 |
<r2> (average value of r
2) Å
2
| <r2> |
47.471 |
| (<r2>)1/2 |
6.890 |