Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -1816.608818 |
| Energy at 298.15K | -1816.610067 |
| Nuclear repulsion energy | 64.639854 |
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/6-311G**
| 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 |
3198 |
2905 |
114.95 |
|
|
|
| 2 |
A1 |
1347 |
1224 |
250.67 |
|
|
|
| 3 |
A1 |
431 |
392 |
0.39 |
|
|
|
| 4 |
B1 |
607 |
551 |
96.55 |
|
|
|
| 5 |
B2 |
3296 |
2994 |
39.08 |
|
|
|
| 6 |
B2 |
531 |
483 |
31.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4704.7 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 4274.2 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 HF/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.458 |
| C2 |
0.000 |
0.000 |
-1.569 |
| H3 |
0.000 |
0.908 |
-2.157 |
| H4 |
0.000 |
-0.908 |
-2.157 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.0263 | 2.7675 | 2.7675 |
C2 | 2.0263 | | 1.0820 | 1.0820 | H3 | 2.7675 | 1.0820 | | 1.8166 | H4 | 2.7675 | 1.0820 | 1.8166 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Zn1 |
C2 |
H3 |
122.913 |
|
Zn1 |
C2 |
H4 |
122.913 |
| H3 |
C2 |
H4 |
114.174 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.520 |
|
|
|
| 2 |
C |
-0.778 |
|
|
|
| 3 |
H |
0.129 |
|
|
|
| 4 |
H |
0.129 |
|
|
|
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 |
1.942 |
1.942 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.881 |
0.000 |
0.000 |
| y |
0.000 |
-21.285 |
0.000 |
| z |
0.000 |
0.000 |
-23.697 |
|
| Traceless |
| | x | y | z |
| x |
-0.390 |
0.000 |
0.000 |
| y |
0.000 |
2.004 |
0.000 |
| z |
0.000 |
0.000 |
-1.613 |
|
| Polar |
| 3z2-r2 | -3.227 |
| x2-y2 | -1.596 |
| 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 |
1.545 |
0.000 |
0.000 |
| y |
0.000 |
2.491 |
0.000 |
| z |
0.000 |
0.000 |
8.342 |
<r2> (average value of r
2) Å
2
| <r2> |
46.129 |
| (<r2>)1/2 |
6.792 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -1816.608818 |
| Energy at 298.15K | -1816.610067 |
| Nuclear repulsion energy | 64.639854 |
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/6-311G**
Geometric Data calculated at HF/6-311G**
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -1816.512412 |
| Energy at 298.15K | -1816.513719 |
| Nuclear repulsion energy | 64.150971 |
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/6-311G**
| 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 |
3349 |
3042 |
1.04 |
|
|
|
| 2 |
A1 |
1111 |
1009 |
896.91 |
|
|
|
| 3 |
A1 |
247 |
224 |
147.90 |
|
|
|
| 4 |
B1 |
5452 |
4953 |
13485.01 |
|
|
|
| 5 |
B2 |
3646 |
3313 |
48.19 |
|
|
|
| 6 |
B2 |
698 |
634 |
36.96 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7250.8 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 6587.4 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/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.454 |
| C2 |
0.000 |
0.000 |
-1.636 |
| H3 |
0.000 |
1.025 |
-1.908 |
| H4 |
0.000 |
-1.025 |
-1.908 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.0901 | 2.5748 | 2.5748 |
C2 | 2.0901 | | 1.0605 | 1.0605 | H3 | 2.5748 | 1.0605 | | 2.0502 | H4 | 2.5748 | 1.0605 | 2.0502 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.492 |
|
|
|
| 2 |
C |
-0.913 |
|
|
|
| 3 |
H |
0.210 |
|
|
|
| 4 |
H |
0.210 |
|
|
|
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 |
4.069 |
4.069 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.674 |
0.000 |
0.000 |
| y |
0.000 |
-19.039 |
0.000 |
| z |
0.000 |
0.000 |
-23.757 |
|
| Traceless |
| | x | y | z |
| x |
-3.276 |
0.000 |
0.000 |
| y |
0.000 |
5.176 |
0.000 |
| z |
0.000 |
0.000 |
-1.901 |
|
| Polar |
| 3z2-r2 | -3.801 |
| x2-y2 | -5.635 |
| 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 |
0.789 |
0.000 |
0.000 |
| y |
0.000 |
2.212 |
0.000 |
| z |
0.000 |
0.000 |
11.324 |
<r2> (average value of r
2) Å
2
| <r2> |
45.672 |
| (<r2>)1/2 |
6.758 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/6-311G**
| | hartrees |
| Energy at 0K | -1816.566254 |
| Energy at 298.15K | -1816.567261 |
| Nuclear repulsion energy | 58.168816 |
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/6-311G**
| 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' |
3070 |
2789 |
86.27 |
|
|
|
| 2 |
A' |
1496 |
1359 |
1.63 |
|
|
|
| 3 |
A' |
672 |
610 |
360.83 |
|
|
|
| 4 |
A' |
163 |
148 |
17.32 |
|
|
|
| 5 |
A" |
3127 |
2841 |
99.38 |
|
|
|
| 6 |
A" |
602 |
547 |
18.91 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4565.0 cm
-1
Scaled (by 0.9085) Zero Point Vibrational Energy (zpe) 4147.3 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.
Geometric Data calculated at HF/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
-0.035 |
-0.504 |
0.000 |
| C2 |
-0.035 |
1.848 |
0.000 |
| H3 |
0.629 |
2.012 |
0.862 |
| H4 |
0.629 |
2.012 |
-0.862 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.3514 | 2.7412 | 2.7412 |
C2 | 2.3514 | | 1.1005 | 1.1005 | H3 | 2.7412 | 1.1005 | | 1.7234 | H4 | 2.7412 | 1.1005 | 1.7234 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.266 |
|
|
|
| 2 |
C |
-0.488 |
|
|
|
| 3 |
H |
0.111 |
|
|
|
| 4 |
H |
0.111 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.588 |
-1.744 |
0.000 |
2.359 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.691 |
3.135 |
0.000 |
| y |
3.135 |
-22.688 |
0.000 |
| z |
0.000 |
0.000 |
-21.876 |
|
| Traceless |
| | x | y | z |
| x |
-1.409 |
3.135 |
0.000 |
| y |
3.135 |
0.096 |
0.000 |
| z |
0.000 |
0.000 |
1.313 |
|
| Polar |
| 3z2-r2 | 2.626 |
| x2-y2 | -1.003 |
| xy | 3.135 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.211 |
0.433 |
0.000 |
| y |
0.433 |
13.477 |
0.000 |
| z |
0.000 |
0.000 |
2.589 |
<r2> (average value of r
2) Å
2
| <r2> |
52.726 |
| (<r2>)1/2 |
7.261 |