Jump to
S1C2
S2C1
S2C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1818.501699 |
| Energy at 298.15K | -1818.502917 |
| Nuclear repulsion energy | 65.219343 |
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 B3LYP/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 |
3073 |
2970 |
47.87 |
|
|
|
| 2 |
A1 |
1284 |
1241 |
89.55 |
|
|
|
| 3 |
A1 |
425 |
411 |
4.21 |
|
|
|
| 4 |
B1 |
585 |
566 |
99.56 |
|
|
|
| 5 |
B2 |
3195 |
3087 |
30.00 |
|
|
|
| 6 |
B2 |
526 |
509 |
23.52 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4544.5 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4391.4 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 B3LYP/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.452 |
| C2 |
0.000 |
0.000 |
-1.552 |
| H3 |
0.000 |
0.924 |
-2.128 |
| H4 |
0.000 |
-0.924 |
-2.128 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.0045 | 2.7412 | 2.7412 |
C2 | 2.0045 | | 1.0890 | 1.0890 | H3 | 2.7412 | 1.0890 | | 1.8480 | H4 | 2.7412 | 1.0890 | 1.8480 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Zn1 |
C2 |
H3 |
121.949 |
|
Zn1 |
C2 |
H4 |
121.949 |
| H3 |
C2 |
H4 |
116.103 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.430 |
|
|
|
| 2 |
C |
-0.881 |
|
|
|
| 3 |
H |
0.226 |
|
|
|
| 4 |
H |
0.226 |
|
|
|
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 |
1.337 |
1.337 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.645 |
0.000 |
0.000 |
| y |
0.000 |
-20.843 |
0.000 |
| z |
0.000 |
0.000 |
-22.689 |
|
| Traceless |
| | x | y | z |
| x |
-0.879 |
0.000 |
0.000 |
| y |
0.000 |
1.824 |
0.000 |
| z |
0.000 |
0.000 |
-0.945 |
|
| Polar |
| 3z2-r2 | -1.890 |
| x2-y2 | -1.802 |
| 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 |
1.537 |
0.000 |
0.000 |
| y |
0.000 |
2.537 |
0.000 |
| z |
0.000 |
0.000 |
7.298 |
<r2> (average value of r
2) Å
2
| <r2> |
45.139 |
| (<r2>)1/2 |
6.719 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1818.501699 |
| Energy at 298.15K | -1818.502917 |
| Nuclear repulsion energy | 65.219343 |
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 B3LYP/6-311G*
Geometric Data calculated at B3LYP/6-311G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1818.446019 |
| Energy at 298.15K | -1818.447572 |
| Nuclear repulsion energy | 68.691273 |
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 B3LYP/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 |
3174 |
3067 |
1.08 |
|
|
|
| 2 |
A1 |
1148 |
1109 |
332.99 |
|
|
|
| 3 |
A1 |
490 |
474 |
6.16 |
|
|
|
| 4 |
B1 |
1392 |
1345 |
1048.23 |
|
|
|
| 5 |
B2 |
3417 |
3302 |
7.58 |
|
|
|
| 6 |
B2 |
706 |
683 |
40.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 5163.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4989.7 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 B3LYP/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.422 |
| C2 |
0.000 |
0.000 |
-1.493 |
| H3 |
0.000 |
1.013 |
-1.848 |
| H4 |
0.000 |
-1.013 |
-1.848 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.9148 | 2.4860 | 2.4860 |
C2 | 1.9148 | | 1.0738 | 1.0738 | H3 | 2.4860 | 1.0738 | | 2.0265 | H4 | 2.4860 | 1.0738 | 2.0265 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.620 |
|
|
|
| 2 |
C |
-1.135 |
|
|
|
| 3 |
H |
0.258 |
|
|
|
| 4 |
H |
0.258 |
|
|
|
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 |
4.753 |
4.753 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.094 |
0.000 |
0.000 |
| y |
0.000 |
-18.699 |
0.000 |
| z |
0.000 |
0.000 |
-23.107 |
|
| Traceless |
| | x | y | z |
| x |
-3.191 |
0.000 |
0.000 |
| y |
0.000 |
4.902 |
0.000 |
| z |
0.000 |
0.000 |
-1.711 |
|
| Polar |
| 3z2-r2 | -3.421 |
| x2-y2 | -5.395 |
| 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 |
1.851 |
0.000 |
0.000 |
| y |
0.000 |
2.379 |
0.000 |
| z |
0.000 |
0.000 |
8.233 |
<r2> (average value of r
2) Å
2
| <r2> |
41.318 |
| (<r2>)1/2 |
6.428 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1818.492397 |
| Energy at 298.15K | -1818.493772 |
| Nuclear repulsion energy | 65.783640 |
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 B3LYP/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' |
2871 |
2775 |
118.20 |
|
|
|
| 2 |
A' |
1441 |
1393 |
1.31 |
|
|
|
| 3 |
A' |
747 |
722 |
289.19 |
|
|
|
| 4 |
A' |
397 |
383 |
2.14 |
|
|
|
| 5 |
A" |
2928 |
2829 |
134.70 |
|
|
|
| 6 |
A" |
692 |
669 |
14.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4537.7 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 4384.8 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.
Geometric Data calculated at B3LYP/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
-0.035 |
-0.438 |
0.000 |
| C2 |
-0.035 |
1.583 |
0.000 |
| H3 |
0.626 |
1.825 |
0.863 |
| H4 |
0.626 |
1.825 |
-0.863 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 2.0209 | 2.5112 | 2.5112 |
C2 | 2.0209 | | 1.1140 | 1.1140 | H3 | 2.5112 | 1.1140 | | 1.7269 | H4 | 2.5112 | 1.1140 | 1.7269 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.489 |
|
|
|
| 2 |
C |
-0.883 |
|
|
|
| 3 |
H |
0.197 |
|
|
|
| 4 |
H |
0.197 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.236 |
-3.004 |
0.000 |
3.248 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.702 |
2.470 |
0.000 |
| y |
2.470 |
-23.256 |
0.000 |
| z |
0.000 |
0.000 |
-21.066 |
|
| Traceless |
| | x | y | z |
| x |
-0.541 |
2.470 |
0.000 |
| y |
2.470 |
-1.372 |
0.000 |
| z |
0.000 |
0.000 |
1.913 |
|
| Polar |
| 3z2-r2 | 3.825 |
| x2-y2 | 0.554 |
| xy | 2.470 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.463 |
0.265 |
0.000 |
| y |
0.265 |
11.368 |
0.000 |
| z |
0.000 |
0.000 |
2.768 |
<r2> (average value of r
2) Å
2
| <r2> |
43.727 |
| (<r2>)1/2 |
6.613 |