Vibrational Frequencies calculated at BLYP/3-21G*
| 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 |
2963 |
2944 |
17.89 |
|
|
|
| 2 |
A1 |
1300 |
1292 |
0.05 |
|
|
|
| 3 |
A1 |
662 |
658 |
11.86 |
|
|
|
| 4 |
E |
3022 |
3003 |
14.30 |
|
|
|
| 4 |
E |
3022 |
3003 |
14.31 |
|
|
|
| 5 |
E |
1444 |
1435 |
10.06 |
|
|
|
| 5 |
E |
1444 |
1435 |
10.05 |
|
|
|
| 6 |
E |
654 |
649 |
1.55 |
|
|
|
| 6 |
E |
654 |
649 |
1.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7583.1 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 7533.8 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 BLYP/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.286 |
|
|
|
| 2 |
C |
-0.935 |
|
|
|
| 3 |
H |
0.216 |
|
|
|
| 4 |
H |
0.216 |
|
|
|
| 5 |
H |
0.216 |
|
|
|
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 |
-0.677 |
0.677 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.033 |
0.000 |
0.000 |
| y |
0.000 |
-22.033 |
0.000 |
| z |
0.000 |
0.000 |
-25.606 |
|
| Traceless |
| | x | y | z |
| x |
1.786 |
0.000 |
0.000 |
| y |
0.000 |
1.786 |
0.000 |
| z |
0.000 |
0.000 |
-3.573 |
|
| Polar |
| 3z2-r2 | -7.146 |
| 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 |
7.240 |
0.000 |
0.000 |
| y |
0.000 |
7.243 |
-0.001 |
| z |
0.000 |
-0.001 |
8.306 |
<r2> (average value of r
2) Å
2
| <r2> |
44.773 |
| (<r2>)1/2 |
6.691 |