Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1816.450627 |
| Energy at 298.15K | -1816.452000 |
| Nuclear repulsion energy | 66.308793 |
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 HF/6-31G(2df,p)
| 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 |
3213 |
2910 |
48.18 |
|
|
|
| 2 |
A1 |
1459 |
1322 |
24.85 |
|
|
|
| 3 |
A1 |
555 |
503 |
27.67 |
|
|
|
| 4 |
B1 |
628 |
569 |
69.00 |
|
|
|
| 5 |
B2 |
3300 |
2988 |
19.32 |
|
|
|
| 6 |
B2 |
552 |
500 |
1.69 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4854.3 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 4395.6 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 HF/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.445 |
| C2 |
0.000 |
0.000 |
-1.519 |
| H3 |
0.000 |
0.898 |
-2.124 |
| H4 |
0.000 |
-0.898 |
-2.124 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.9647 | 2.7217 | 2.7217 |
C2 | 1.9647 | | 1.0823 | 1.0823 | H3 | 2.7217 | 1.0823 | | 1.7952 | H4 | 2.7217 | 1.0823 | 1.7952 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Zn1 |
C2 |
H3 |
123.968 |
|
Zn1 |
C2 |
H4 |
123.968 |
| H3 |
C2 |
H4 |
112.065 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.417 |
|
|
|
| 2 |
C |
-0.702 |
|
|
|
| 3 |
H |
0.143 |
|
|
|
| 4 |
H |
0.143 |
|
|
|
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 |
0.127 |
0.127 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-21.825 |
0.000 |
0.000 |
| y |
0.000 |
-20.262 |
0.000 |
| z |
0.000 |
0.000 |
-25.316 |
|
| Traceless |
| | x | y | z |
| x |
0.964 |
0.000 |
0.000 |
| y |
0.000 |
3.308 |
0.000 |
| z |
0.000 |
0.000 |
-4.272 |
|
| Polar |
| 3z2-r2 | -8.545 |
| x2-y2 | -1.563 |
| 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 |
6.217 |
0.000 |
0.000 |
| y |
0.000 |
7.254 |
0.000 |
| z |
0.000 |
0.000 |
7.386 |
<r2> (average value of r
2) Å
2
| <r2> |
44.469 |
| (<r2>)1/2 |
6.668 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1816.450627 |
| Energy at 298.15K | -1816.452000 |
| Nuclear repulsion energy | 66.308793 |
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 HF/6-31G(2df,p)
Geometric Data calculated at HF/6-31G(2df,p)
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1816.357608 |
| Energy at 298.15K | -1816.359318 |
| Nuclear repulsion energy | 71.432496 |
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 HF/6-31G(2df,p)
| 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 |
3299 |
2987 |
2.44 |
|
|
|
| 2 |
A1 |
1267 |
1147 |
176.14 |
|
|
|
| 3 |
A1 |
736 |
666 |
1.51 |
|
|
|
| 4 |
B1 |
6599 |
5976 |
0.00 |
|
|
|
| 5 |
B2 |
3457 |
3130 |
6.12 |
|
|
|
| 6 |
B2 |
683 |
619 |
115.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8020.5 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 7262.6 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 HF/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.408 |
| C2 |
0.000 |
0.000 |
-1.404 |
| H3 |
0.000 |
0.944 |
-1.911 |
| H4 |
0.000 |
-0.944 |
-1.911 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.8127 | 2.5040 | 2.5040 |
C2 | 1.8127 | | 1.0716 | 1.0716 | H3 | 2.5040 | 1.0716 | | 1.8890 | H4 | 2.5040 | 1.0716 | 1.8890 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.494 |
|
|
|
| 2 |
C |
-0.824 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
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 |
4.812 |
4.812 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.453 |
0.000 |
0.000 |
| y |
0.000 |
-19.314 |
0.000 |
| z |
0.000 |
0.000 |
-20.081 |
|
| Traceless |
| | x | y | z |
| x |
-6.756 |
0.000 |
0.000 |
| y |
0.000 |
3.953 |
0.000 |
| z |
0.000 |
0.000 |
2.803 |
|
| Polar |
| 3z2-r2 | 5.606 |
| x2-y2 | -7.139 |
| 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 |
6.217 |
0.000 |
0.000 |
| y |
0.000 |
7.254 |
0.000 |
| z |
0.000 |
0.000 |
7.386 |
<r2> (average value of r
2) Å
2
| <r2> |
39.630 |
| (<r2>)1/2 |
6.295 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1816.388852 |
| Energy at 298.15K | -1816.390217 |
| Nuclear repulsion energy | 65.626436 |
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 HF/6-31G(2df,p)
| 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' |
3111 |
2817 |
32.20 |
|
|
|
| 2 |
A' |
1489 |
1348 |
2.84 |
|
|
|
| 3 |
A' |
761 |
689 |
661.00 |
|
|
|
| 4 |
A' |
377 |
341 |
38.63 |
|
|
|
| 5 |
A" |
3180 |
2879 |
17.00 |
|
|
|
| 6 |
A" |
692 |
627 |
92.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4804.7 cm
-1
Scaled (by 0.9055) Zero Point Vibrational Energy (zpe) 4350.6 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 HF/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
-0.032 |
-0.441 |
0.000 |
| C2 |
-0.032 |
1.587 |
0.000 |
| H3 |
0.581 |
1.854 |
0.868 |
| H4 |
0.581 |
1.854 |
-0.868 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.0278 | 2.5288 | 2.5288 |
C2 | 2.0278 | | 1.0960 | 1.0960 | H3 | 2.5288 | 1.0960 | | 1.7367 | H4 | 2.5288 | 1.0960 | 1.7367 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.321 |
|
|
|
| 2 |
C |
-0.650 |
|
|
|
| 3 |
H |
0.165 |
|
|
|
| 4 |
H |
0.165 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.255 |
-1.486 |
0.000 |
1.508 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.298 |
3.546 |
0.000 |
| y |
3.546 |
-22.881 |
0.000 |
| z |
0.000 |
0.000 |
-21.067 |
|
| Traceless |
| | x | y | z |
| x |
-1.324 |
3.546 |
0.000 |
| y |
3.546 |
-0.698 |
0.000 |
| z |
0.000 |
0.000 |
2.023 |
|
| Polar |
| 3z2-r2 | 4.045 |
| x2-y2 | -0.417 |
| xy | 3.546 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.195 |
-0.678 |
0.000 |
| y |
-0.678 |
18.311 |
0.000 |
| z |
0.000 |
0.000 |
7.224 |
<r2> (average value of r
2) Å
2
| <r2> |
44.035 |
| (<r2>)1/2 |
6.636 |