Jump to
S2C1
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -487.496105 |
| Energy at 298.15K | -487.376418 |
| HF Energy | -487.496105 |
| Nuclear repulsion energy | 101.194255 |
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/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.572 |
| F2 |
0.000 |
1.226 |
-0.445 |
| F3 |
0.000 |
-1.226 |
-0.445 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.5930 | 1.5930 |
F2 | 1.5930 | | 2.4519 | F3 | 1.5930 | 2.4519 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
100.636 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.159 |
|
|
|
| 2 |
F |
-0.079 |
|
|
|
| 3 |
F |
-0.079 |
|
|
|
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 |
0.677 |
0.677 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.974 |
0.000 |
0.000 |
| y |
0.000 |
-23.606 |
0.000 |
| z |
0.000 |
0.000 |
-22.862 |
|
| Traceless |
| | x | y | z |
| x |
3.260 |
0.000 |
0.000 |
| y |
0.000 |
-2.188 |
0.000 |
| z |
0.000 |
0.000 |
-1.072 |
|
| Polar |
| 3z2-r2 | -2.143 |
| x2-y2 | 3.632 |
| 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 |
3.954 |
0.000 |
0.000 |
| y |
0.000 |
4.091 |
0.000 |
| z |
0.000 |
0.000 |
3.588 |
<r2> (average value of r
2) Å
2
| <r2> |
49.034 |
| (<r2>)1/2 |
7.002 |
Jump to
S1C1
Energy calculated at LSDA/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -487.373414 |
| Energy at 298.15K | -487.253635 |
| HF Energy | -487.373414 |
| Nuclear repulsion energy | 99.732560 |
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/6-31G(2df,p)
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.151 |
|
|
|
| 2 |
F |
-0.075 |
|
|
|
| 3 |
F |
-0.075 |
|
|
|
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 |
1.014 |
1.014 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.958 |
0.000 |
0.000 |
| y |
0.000 |
-23.466 |
0.000 |
| z |
0.000 |
0.000 |
-20.607 |
|
| Traceless |
| | x | y | z |
| x |
-0.922 |
0.000 |
0.000 |
| y |
0.000 |
-1.684 |
0.000 |
| z |
0.000 |
0.000 |
2.605 |
|
| Polar |
| 3z2-r2 | 5.210 |
| x2-y2 | 0.508 |
| 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 |
3.757 |
0.000 |
0.000 |
| y |
0.000 |
3.715 |
0.000 |
| z |
0.000 |
0.000 |
3.275 |
<r2> (average value of r
2) Å
2
| <r2> |
52.045 |
| (<r2>)1/2 |
7.214 |