Jump to
S2C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -489.182649 |
| Energy at 298.15K | |
| HF Energy | -488.957213 |
| Nuclear repulsion energy | 99.909891 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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 |
835 |
801 |
133.00 |
4.65 |
0.54 |
0.70 |
| 2 |
A1 |
335 |
321 |
17.63 |
0.85 |
0.13 |
0.24 |
| 3 |
B2 |
845 |
811 |
177.29 |
6.25 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1007.4 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 966.2 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.583 |
| F2 |
0.000 |
1.238 |
-0.453 |
| F3 |
0.000 |
-1.238 |
-0.453 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6144 | 1.6144 |
F2 | 1.6144 | | 2.4762 | F3 | 1.6144 | 2.4762 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
100.150 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.869 |
|
|
|
| 2 |
F |
-0.434 |
|
|
|
| 3 |
F |
-0.434 |
|
|
|
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 |
1.292 |
1.292 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-20.056 |
0.000 |
0.000 |
| y |
0.000 |
-25.301 |
0.000 |
| z |
0.000 |
0.000 |
-23.735 |
|
| Traceless |
| | x | y | z |
| x |
4.462 |
0.000 |
0.000 |
| y |
0.000 |
-3.405 |
0.000 |
| z |
0.000 |
0.000 |
-1.057 |
|
| Polar |
| 3z2-r2 | -2.114 |
| x2-y2 | 5.245 |
| 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 |
4.341 |
0.000 |
0.000 |
| y |
0.000 |
4.487 |
0.000 |
| z |
0.000 |
0.000 |
4.110 |
<r2> (average value of r
2) Å
2
| <r2> |
50.434 |
| (<r2>)1/2 |
7.102 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -489.065741 |
| Energy at 298.15K | |
| HF Energy | -488.850449 |
| Nuclear repulsion energy | 98.746175 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.497 |
| F2 |
0.000 |
1.346 |
-0.386 |
| F3 |
0.000 |
-1.346 |
-0.386 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6101 | 1.6101 |
F2 | 1.6101 | | 2.6922 | F3 | 1.6101 | 2.6922 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
113.452 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.832 |
|
|
|
| 2 |
F |
-0.416 |
|
|
|
| 3 |
F |
-0.416 |
|
|
|
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 |
1.318 |
1.318 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-23.578 |
0.000 |
0.000 |
| y |
0.000 |
-25.242 |
0.000 |
| z |
0.000 |
0.000 |
-21.377 |
|
| Traceless |
| | x | y | z |
| x |
-0.268 |
0.000 |
0.000 |
| y |
0.000 |
-2.765 |
0.000 |
| z |
0.000 |
0.000 |
3.033 |
|
| Polar |
| 3z2-r2 | 6.066 |
| x2-y2 | 1.664 |
| 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 |
5.507 |
0.000 |
0.000 |
| y |
0.000 |
4.534 |
0.000 |
| z |
0.000 |
0.000 |
4.272 |
<r2> (average value of r
2) Å
2
| <r2> |
53.380 |
| (<r2>)1/2 |
7.306 |