Jump to
S2C1
Energy calculated at MP2=FULL/6-311G*
| | hartrees |
| Energy at 0K | -488.603857 |
| Energy at 298.15K | |
| HF Energy | -487.953266 |
| Nuclear repulsion energy | 99.868441 |
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 MP2=FULL/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 |
868 |
822 |
138.02 |
4.06 |
0.60 |
0.75 |
| 2 |
A1 |
349 |
331 |
23.03 |
0.88 |
0.40 |
0.58 |
| 3 |
B2 |
885 |
838 |
174.05 |
5.16 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1050.9 cm
-1
Scaled (by 0.9471) Zero Point Vibrational Energy (zpe) 995.3 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 MP2=FULL/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.581 |
| F2 |
0.000 |
1.241 |
-0.452 |
| F3 |
0.000 |
-1.241 |
-0.452 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6145 | 1.6145 |
F2 | 1.6145 | | 2.4816 | F3 | 1.6145 | 2.4816 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
100.446 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
Energy calculated at MP2=FULL/6-311G*
| | hartrees |
| Energy at 0K | -488.490640 |
| Energy at 298.15K | -488.370882 |
| HF Energy | -487.865215 |
| Nuclear repulsion energy | 98.408989 |
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 MP2=FULL/6-311G*
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability