Jump to
S2C1
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -487.562948 |
| Energy at 298.15K | -487.443236 |
| HF Energy | -487.562948 |
| Nuclear repulsion energy | 99.830894 |
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 LSDA/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.585 |
| F2 |
0.000 |
1.237 |
-0.455 |
| F3 |
0.000 |
-1.237 |
-0.455 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6163 | 1.6163 |
F2 | 1.6163 | | 2.4736 | F3 | 1.6163 | 2.4736 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
99.849 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.707 |
|
|
|
| 2 |
F |
-0.354 |
|
|
|
| 3 |
F |
-0.354 |
|
|
|
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 |
1.275 |
1.275 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.635 |
0.000 |
0.000 |
| y |
0.000 |
-24.929 |
0.000 |
| z |
0.000 |
0.000 |
-23.015 |
|
| Traceless |
| | x | y | z |
| x |
4.337 |
0.000 |
0.000 |
| y |
0.000 |
-3.604 |
0.000 |
| z |
0.000 |
0.000 |
-0.732 |
|
| Polar |
| 3z2-r2 | -1.465 |
| x2-y2 | 5.294 |
| 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 |
3.376 |
0.000 |
0.000 |
| y |
0.000 |
3.876 |
0.000 |
| z |
0.000 |
0.000 |
3.187 |
<r2> (average value of r
2) Å
2
| <r2> |
50.132 |
| (<r2>)1/2 |
7.080 |
Jump to
S1C1
Energy calculated at LSDA/6-311G*
| | hartrees |
| Energy at 0K | -487.439548 |
| Energy at 298.15K | -487.319737 |
| HF Energy | -487.439548 |
| Nuclear repulsion energy | 98.187027 |
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 LSDA/6-311G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.659 |
|
|
|
| 2 |
F |
-0.330 |
|
|
|
| 3 |
F |
-0.330 |
|
|
|
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 |
1.642 |
1.642 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.016 |
0.000 |
0.000 |
| y |
0.000 |
-25.131 |
0.000 |
| z |
0.000 |
0.000 |
-20.460 |
|
| Traceless |
| | x | y | z |
| x |
-0.221 |
0.000 |
0.000 |
| y |
0.000 |
-3.392 |
0.000 |
| z |
0.000 |
0.000 |
3.614 |
|
| Polar |
| 3z2-r2 | 7.227 |
| x2-y2 | 2.114 |
| 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 |
2.653 |
0.000 |
0.000 |
| y |
0.000 |
3.357 |
0.000 |
| z |
0.000 |
0.000 |
2.642 |
<r2> (average value of r
2) Å
2
| <r2> |
53.711 |
| (<r2>)1/2 |
7.329 |