Jump to
S1C2
S2C1
S2C2
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -1807.216487 |
| Energy at 298.15K | -1807.218075 |
| Nuclear repulsion energy | 73.124833 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/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 |
3062 |
3006 |
7.41 |
|
|
|
| 2 |
A1 |
1365 |
1341 |
0.01 |
|
|
|
| 3 |
A1 |
760 |
747 |
12.62 |
|
|
|
| 4 |
B1 |
779 |
765 |
115.35 |
|
|
|
| 5 |
B2 |
3162 |
3105 |
2.64 |
|
|
|
| 6 |
B2 |
635 |
624 |
2.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4881.5 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 4793.7 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.
Geometric Data calculated at LSDA/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.400 |
| C2 |
0.000 |
0.000 |
-1.349 |
| H3 |
0.000 |
0.917 |
-1.950 |
| H4 |
0.000 |
-0.917 |
-1.950 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.7489 | 2.5230 | 2.5230 |
C2 | 1.7489 | | 1.0970 | 1.0970 | H3 | 2.5230 | 1.0970 | | 1.8350 | H4 | 2.5230 | 1.0970 | 1.8350 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Zn1 |
C2 |
H3 |
123.240 |
|
Zn1 |
C2 |
H4 |
123.240 |
| H3 |
C2 |
H4 |
113.521 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.315 |
|
|
|
| 2 |
C |
-0.770 |
|
|
|
| 3 |
H |
0.228 |
|
|
|
| 4 |
H |
0.228 |
|
|
|
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 |
-0.636 |
0.636 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.998 |
0.000 |
0.000 |
| y |
0.000 |
-20.570 |
0.000 |
| z |
0.000 |
0.000 |
-23.354 |
|
| Traceless |
| | x | y | z |
| x |
-1.036 |
0.000 |
0.000 |
| y |
0.000 |
2.606 |
0.000 |
| z |
0.000 |
0.000 |
-1.570 |
|
| Polar |
| 3z2-r2 | -3.140 |
| x2-y2 | -2.428 |
| 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 |
5.666 |
0.000 |
0.000 |
| y |
0.000 |
6.580 |
0.000 |
| z |
0.000 |
0.000 |
7.692 |
<r2> (average value of r
2) Å
2
| <r2> |
38.941 |
| (<r2>)1/2 |
6.240 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -1807.216487 |
| Energy at 298.15K | -1807.218075 |
| Nuclear repulsion energy | 73.124833 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/3-21G*
Geometric Data calculated at LSDA/3-21G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C2
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -1807.206194 |
| Energy at 298.15K | |
| Nuclear repulsion energy | 76.763943 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/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 |
3146 |
3089 |
21.85 |
|
|
|
| 2 |
A1 |
1327 |
1303 |
46.47 |
|
|
|
| 3 |
A1 |
885 |
869 |
13.86 |
|
|
|
| 4 |
B1 |
818i |
803i |
292.06 |
|
|
|
| 5 |
B2 |
3315 |
3256 |
13.68 |
|
|
|
| 6 |
B2 |
792 |
778 |
89.35 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4323.8 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 4246.0 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.
Geometric Data calculated at LSDA/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.376 |
| C2 |
0.000 |
0.000 |
-1.289 |
| H3 |
0.000 |
0.970 |
-1.776 |
| H4 |
0.000 |
-0.970 |
-1.776 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.6654 | 2.3611 | 2.3611 |
C2 | 1.6654 | | 1.0856 | 1.0856 | H3 | 2.3611 | 1.0856 | | 1.9403 | H4 | 2.3611 | 1.0856 | 1.9403 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.391 |
|
|
|
| 2 |
C |
-0.878 |
|
|
|
| 3 |
H |
0.244 |
|
|
|
| 4 |
H |
0.244 |
|
|
|
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 |
2.827 |
2.827 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-27.072 |
0.000 |
0.000 |
| y |
0.000 |
-19.572 |
0.000 |
| z |
0.000 |
0.000 |
-19.404 |
|
| Traceless |
| | x | y | z |
| x |
-7.584 |
0.000 |
0.000 |
| y |
0.000 |
3.666 |
0.000 |
| z |
0.000 |
0.000 |
3.918 |
|
| Polar |
| 3z2-r2 | 7.837 |
| x2-y2 | -7.500 |
| 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 |
9.407 |
0.000 |
0.000 |
| y |
0.000 |
4.226 |
0.000 |
| z |
0.000 |
0.000 |
8.024 |
<r2> (average value of r
2) Å
2
| <r2> |
36.162 |
| (<r2>)1/2 |
6.014 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at LSDA/3-21G*
| | hartrees |
| Energy at 0K | -1807.212503 |
| Energy at 298.15K | -1807.214118 |
| Nuclear repulsion energy | 75.218072 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/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 |
A' |
2948 |
2895 |
22.02 |
|
|
|
| 2 |
A' |
1331 |
1307 |
49.56 |
|
|
|
| 3 |
A' |
777 |
763 |
15.25 |
|
|
|
| 4 |
A' |
702 |
689 |
148.79 |
|
|
|
| 5 |
A" |
3038 |
2983 |
3.04 |
|
|
|
| 6 |
A" |
753 |
739 |
52.58 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4774.2 cm
-1
Scaled (by 0.982) Zero Point Vibrational Energy (zpe) 4688.2 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.
Geometric Data calculated at LSDA/3-21G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
-0.026 |
-0.381 |
0.000 |
| C2 |
-0.026 |
1.328 |
0.000 |
| H3 |
0.470 |
1.738 |
0.904 |
| H4 |
0.470 |
1.738 |
-0.904 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.7091 | 2.3568 | 2.3568 |
C2 | 1.7091 | | 1.1100 | 1.1100 | H3 | 2.3568 | 1.1100 | | 1.8082 | H4 | 2.3568 | 1.1100 | 1.8082 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.349 |
|
|
|
| 2 |
C |
-0.815 |
|
|
|
| 3 |
H |
0.233 |
|
|
|
| 4 |
H |
0.233 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.056 |
-1.855 |
0.000 |
1.856 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.563 |
4.278 |
0.000 |
| y |
4.278 |
-22.009 |
0.000 |
| z |
0.000 |
0.000 |
-20.460 |
|
| Traceless |
| | x | y | z |
| x |
-3.329 |
4.278 |
0.000 |
| y |
4.278 |
0.503 |
0.000 |
| z |
0.000 |
0.000 |
2.826 |
|
| Polar |
| 3z2-r2 | 5.652 |
| x2-y2 | -2.555 |
| xy | 4.278 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.876 |
-1.073 |
0.000 |
| y |
-1.073 |
11.351 |
0.000 |
| z |
0.000 |
0.000 |
5.187 |
<r2> (average value of r
2) Å
2
| <r2> |
37.037 |
| (<r2>)1/2 |
6.086 |