Jump to
S2C1
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| | hartrees |
| Energy at 0K | -488.976577 |
| Energy at 298.15K | |
| HF Energy | -488.832798 |
| Nuclear repulsion energy | 99.844466 |
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/6-31G*
| 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 |
877 |
832 |
109.43 |
4.03 |
0.58 |
0.74 |
| 2 |
A1 |
332 |
315 |
18.46 |
0.80 |
0.36 |
0.53 |
| 3 |
B2 |
910 |
863 |
135.13 |
5.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1059.7 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 1005.3 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 B2PLYP=FULLultrafine/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.578 |
| F2 |
0.000 |
1.244 |
-0.450 |
| F3 |
0.000 |
-1.244 |
-0.450 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6140 | 1.6140 |
F2 | 1.6140 | | 2.4887 | F3 | 1.6140 | 2.4887 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
100.877 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.775 |
|
|
|
| 2 |
F |
-0.387 |
|
|
|
| 3 |
F |
-0.387 |
|
|
|
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 |
1.019 |
1.019 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.379 |
0.000 |
0.000 |
| y |
0.000 |
-24.617 |
0.000 |
| z |
0.000 |
0.000 |
-23.139 |
|
| Traceless |
| | x | y | z |
| x |
4.499 |
0.000 |
0.000 |
| y |
0.000 |
-3.357 |
0.000 |
| z |
0.000 |
0.000 |
-1.141 |
|
| Polar |
| 3z2-r2 | -2.283 |
| x2-y2 | 5.237 |
| 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 |
3.512 |
0.000 |
0.000 |
| y |
0.000 |
3.871 |
0.000 |
| z |
0.000 |
0.000 |
3.091 |
<r2> (average value of r
2) Å
2
| <r2> |
50.173 |
| (<r2>)1/2 |
7.083 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/6-31G*
| | hartrees |
| Energy at 0K | -488.856324 |
| Energy at 298.15K | |
| HF Energy | -488.720744 |
| Nuclear repulsion energy | 98.086582 |
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/6-31G*
| 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 |
823 |
781 |
46.63 |
9.12 |
0.30 |
0.46 |
| 2 |
A1 |
268 |
254 |
17.50 |
0.86 |
0.64 |
0.78 |
| 3 |
B2 |
964 |
915 |
119.39 |
6.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1027.4 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 974.7 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/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Si1 |
0.000 |
0.000 |
0.481 |
| F2 |
0.000 |
1.373 |
-0.374 |
| F3 |
0.000 |
-1.373 |
-0.374 |
Atom - Atom Distances (Å)
| |
Si1 |
F2 |
F3 |
| Si1 | | 1.6169 | 1.6169 |
F2 | 1.6169 | | 2.7454 | F3 | 1.6169 | 2.7454 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| F2 |
Si1 |
F3 |
116.202 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Si |
0.731 |
|
|
|
| 2 |
F |
-0.365 |
|
|
|
| 3 |
F |
-0.365 |
|
|
|
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 |
1.628 |
1.628 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-22.630 |
0.000 |
0.000 |
| y |
0.000 |
-24.816 |
0.000 |
| z |
0.000 |
0.000 |
-20.109 |
|
| Traceless |
| | x | y | z |
| x |
-0.168 |
0.000 |
0.000 |
| y |
0.000 |
-3.447 |
0.000 |
| z |
0.000 |
0.000 |
3.614 |
|
| Polar |
| 3z2-r2 | 7.229 |
| x2-y2 | 2.186 |
| 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 |
2.832 |
0.000 |
0.000 |
| y |
0.000 |
3.217 |
0.000 |
| z |
0.000 |
0.000 |
2.504 |
<r2> (average value of r
2) Å
2
| <r2> |
53.734 |
| (<r2>)1/2 |
7.330 |