Jump to
S2C1
S3C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -75.792694 |
| Energy at 298.15K | -75.789668 |
| HF Energy | -75.792694 |
| Nuclear repulsion energy | 15.131124 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HSEh1PBE/cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.630 |
| C2 |
0.000 |
0.000 |
-0.630 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.000 |
|
|
|
| 2 |
C |
0.000 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.118 |
0.000 |
0.000 |
| y |
0.000 |
-12.118 |
0.000 |
| z |
0.000 |
0.000 |
-8.736 |
|
| Traceless |
| | x | y | z |
| x |
-1.691 |
0.000 |
0.000 |
| y |
0.000 |
-1.691 |
0.000 |
| z |
0.000 |
0.000 |
3.382 |
|
| Polar |
| 3z2-r2 | 6.764 |
| x2-y2 | 0.000 |
| 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 |
5.870 |
0.000 |
0.000 |
| y |
0.000 |
5.870 |
0.000 |
| z |
0.000 |
0.000 |
4.590 |
<r2> (average value of r
2) Å
2
| <r2> |
11.620 |
| (<r2>)1/2 |
3.409 |
Jump to
S1C1
S3C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -75.792694 |
| Energy at 298.15K | -75.789668 |
| HF Energy | -75.792694 |
| Nuclear repulsion energy | 15.131124 |
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 HSEh1PBE/cc-pVDZ
Geometric Data calculated at HSEh1PBE/cc-pVDZ
Point Group is D∞h
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
Energy calculated at HSEh1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -75.832643 |
| Energy at 298.15K | -75.829615 |
| HF Energy | -75.832643 |
| Nuclear repulsion energy | 14.496360 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at HSEh1PBE/cc-pVDZ
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.657 |
| C2 |
0.000 |
0.000 |
-0.657 |
Atom - Atom Distances (Å)
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.000 |
|
|
|
| 2 |
C |
0.000 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-12.406 |
0.000 |
0.000 |
| y |
0.000 |
-10.457 |
0.000 |
| z |
0.000 |
0.000 |
-12.074 |
|
| Traceless |
| | x | y | z |
| x |
-1.140 |
0.000 |
0.000 |
| y |
0.000 |
1.783 |
0.000 |
| z |
0.000 |
0.000 |
-0.643 |
|
| Polar |
| 3z2-r2 | -1.285 |
| x2-y2 | -1.949 |
| 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 |
4.042 |
0.000 |
0.000 |
| y |
0.000 |
1.598 |
0.000 |
| z |
0.000 |
0.000 |
6.223 |
<r2> (average value of r
2) Å
2
| <r2> |
12.455 |
| (<r2>)1/2 |
3.529 |