Jump to
S1C2
S2C1
S2C2
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -1815.749945 |
| Energy at 298.15K | -1815.751372 |
| Nuclear repulsion energy | 69.639092 |
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/6-31G*
| 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 |
3055 |
2998 |
8.88 |
|
|
|
| 2 |
A1 |
1312 |
1288 |
5.47 |
|
|
|
| 3 |
A1 |
627 |
616 |
16.94 |
|
|
|
| 4 |
B1 |
671 |
658 |
87.89 |
|
|
|
| 5 |
B2 |
3163 |
3104 |
2.50 |
|
|
|
| 6 |
B2 |
559 |
549 |
2.09 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4693.8 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 4606.0 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/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.421 |
| C2 |
0.000 |
0.000 |
-1.430 |
| H3 |
0.000 |
0.921 |
-2.030 |
| H4 |
0.000 |
-0.921 |
-2.030 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.8512 | 2.6190 | 2.6190 |
C2 | 1.8512 | | 1.0996 | 1.0996 | H3 | 2.6190 | 1.0996 | | 1.8424 | H4 | 2.6190 | 1.0996 | 1.8424 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Zn1 |
C2 |
H3 |
123.099 |
|
Zn1 |
C2 |
H4 |
123.099 |
| H3 |
C2 |
H4 |
113.802 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.210 |
|
|
|
| 2 |
C |
-0.586 |
|
|
|
| 3 |
H |
0.188 |
|
|
|
| 4 |
H |
0.188 |
|
|
|
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 |
-0.734 |
0.734 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.399 |
0.000 |
0.000 |
| y |
0.000 |
-20.245 |
0.000 |
| z |
0.000 |
0.000 |
-22.628 |
|
| Traceless |
| | x | y | z |
| x |
-0.962 |
0.000 |
0.000 |
| y |
0.000 |
2.269 |
0.000 |
| z |
0.000 |
0.000 |
-1.307 |
|
| Polar |
| 3z2-r2 | -2.613 |
| x2-y2 | -2.154 |
| 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 |
5.668 |
0.000 |
0.000 |
| y |
0.000 |
6.623 |
0.000 |
| z |
0.000 |
0.000 |
8.045 |
<r2> (average value of r
2) Å
2
| <r2> |
41.124 |
| (<r2>)1/2 |
6.413 |
Jump to
S1C1
S2C1
S2C2
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -1815.749945 |
| Energy at 298.15K | -1815.751372 |
| Nuclear repulsion energy | 69.639092 |
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/6-31G*
Geometric Data calculated at LSDA/6-31G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
S2C2
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -1815.733427 |
| Energy at 298.15K | |
| Nuclear repulsion energy | 73.893772 |
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/6-31G*
| 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 |
3136 |
3077 |
19.58 |
|
|
|
| 2 |
A1 |
1205 |
1182 |
63.78 |
|
|
|
| 3 |
A1 |
775 |
761 |
7.63 |
|
|
|
| 4 |
B1 |
1383i |
1357i |
1573.85 |
|
|
|
| 5 |
B2 |
3308 |
3246 |
19.06 |
|
|
|
| 6 |
B2 |
694 |
681 |
72.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3867.3 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 3795.0 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/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
0.000 |
0.000 |
0.392 |
| C2 |
0.000 |
0.000 |
-1.350 |
| H3 |
0.000 |
0.981 |
-1.823 |
| H4 |
0.000 |
-0.981 |
-1.823 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.7418 | 2.4223 | 2.4223 |
C2 | 1.7418 | | 1.0892 | 1.0892 | H3 | 2.4223 | 1.0892 | | 1.9624 | H4 | 2.4223 | 1.0892 | 1.9624 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.284 |
|
|
|
| 2 |
C |
-0.682 |
|
|
|
| 3 |
H |
0.199 |
|
|
|
| 4 |
H |
0.199 |
|
|
|
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 |
2.788 |
2.788 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-26.269 |
0.000 |
0.000 |
| y |
0.000 |
-19.120 |
0.000 |
| z |
0.000 |
0.000 |
-19.168 |
|
| Traceless |
| | x | y | z |
| x |
-7.124 |
0.000 |
0.000 |
| y |
0.000 |
3.598 |
0.000 |
| z |
0.000 |
0.000 |
3.526 |
|
| Polar |
| 3z2-r2 | 7.052 |
| x2-y2 | -7.149 |
| 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 |
10.827 |
0.000 |
0.000 |
| y |
0.000 |
4.210 |
0.000 |
| z |
0.000 |
0.000 |
8.474 |
<r2> (average value of r
2) Å
2
| <r2> |
37.551 |
| (<r2>)1/2 |
6.128 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at LSDA/6-31G*
| | hartrees |
| Energy at 0K | -1815.750573 |
| Energy at 298.15K | -1815.752116 |
| Nuclear repulsion energy | 72.203770 |
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/6-31G*
| 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' |
2904 |
2850 |
15.01 |
|
|
|
| 2 |
A' |
1301 |
1276 |
7.84 |
|
|
|
| 3 |
A' |
772 |
758 |
187.74 |
|
|
|
| 4 |
A' |
629 |
617 |
31.04 |
|
|
|
| 5 |
A" |
2990 |
2935 |
10.22 |
|
|
|
| 6 |
A" |
689 |
676 |
47.10 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4642.2 cm
-1
Scaled (by 0.9813) Zero Point Vibrational Energy (zpe) 4555.4 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 LSDA/6-31G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Zn1 |
-0.032 |
-0.396 |
0.000 |
| C2 |
-0.032 |
1.408 |
0.000 |
| H3 |
0.570 |
1.714 |
0.889 |
| H4 |
0.570 |
1.714 |
-0.889 |
Atom - Atom Distances (Å)
| |
Zn1 |
C2 |
H3 |
H4 |
| Zn1 | | 1.8038 | 2.3676 | 2.3676 |
C2 | 1.8038 | | 1.1163 | 1.1163 | H3 | 2.3676 | 1.1163 | | 1.7773 | H4 | 2.3676 | 1.1163 | 1.7773 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Zn |
0.267 |
|
|
|
| 2 |
C |
-0.640 |
|
|
|
| 3 |
H |
0.186 |
|
|
|
| 4 |
H |
0.186 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.132 |
-1.949 |
0.000 |
1.953 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.252 |
3.792 |
0.000 |
| y |
3.792 |
-22.222 |
0.000 |
| z |
0.000 |
0.000 |
-20.263 |
|
| Traceless |
| | x | y | z |
| x |
-2.010 |
3.792 |
0.000 |
| y |
3.792 |
-0.464 |
0.000 |
| z |
0.000 |
0.000 |
2.474 |
|
| Polar |
| 3z2-r2 | 4.948 |
| x2-y2 | -1.030 |
| xy | 3.792 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.557 |
-0.569 |
0.000 |
| y |
-0.569 |
11.169 |
0.000 |
| z |
0.000 |
0.000 |
5.309 |
<r2> (average value of r
2) Å
2
| <r2> |
38.425 |
| (<r2>)1/2 |
6.199 |