Jump to
S2C1
Energy calculated at B3LYP/6-31+G**
| hartrees |
Energy at 0K | -489.283124 |
Energy at 298.15K | |
HF Energy | -489.283124 |
Nuclear repulsion energy | 98.635941 |
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 B3LYP/6-31+G**
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 |
816 |
787 |
149.55 |
4.91 |
0.65 |
0.79 |
2 |
A1 |
319 |
308 |
18.32 |
0.68 |
0.24 |
0.38 |
3 |
B2 |
829 |
799 |
197.12 |
7.90 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 981.9 cm
-1
Scaled (by 0.9642) Zero Point Vibrational Energy (zpe) 946.7 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 B3LYP/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Si1 |
0.000 |
0.000 |
0.589 |
F2 |
0.000 |
1.256 |
-0.458 |
F3 |
0.000 |
-1.256 |
-0.458 |
Atom - Atom Distances (Å)
|
Si1 |
F2 |
F3 |
Si1 | | 1.6348 | 1.6348 |
F2 | 1.6348 | | 2.5116 | F3 | 1.6348 | 2.5116 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Si1 |
F3 |
100.378 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.594 |
|
|
|
2 |
F |
-0.297 |
|
|
|
3 |
F |
-0.297 |
|
|
|
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 |
1.573 |
1.573 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.970 |
0.000 |
0.000 |
y |
0.000 |
-25.738 |
0.000 |
z |
0.000 |
0.000 |
-23.610 |
|
Traceless |
| x | y | z |
x |
4.705 |
0.000 |
0.000 |
y |
0.000 |
-3.948 |
0.000 |
z |
0.000 |
0.000 |
-0.756 |
|
Polar |
3z2-r2 | -1.513 |
x2-y2 | 5.769 |
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 |
3.925 |
0.000 |
0.000 |
y |
0.000 |
4.353 |
0.000 |
z |
0.000 |
0.000 |
3.815 |
<r2> (average value of r
2) Å
2
<r2> |
51.446 |
(<r2>)1/2 |
7.173 |
Jump to
S1C1
Energy calculated at B3LYP/6-31+G**
| hartrees |
Energy at 0K | -489.165205 |
Energy at 298.15K | -489.045390 |
HF Energy | -489.165205 |
Nuclear repulsion energy | 97.370865 |
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 B3LYP/6-31+G**
Point Group is C2v
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.511 |
|
|
|
2 |
F |
-0.256 |
|
|
|
3 |
F |
-0.256 |
|
|
|
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 |
1.720 |
1.720 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-23.532 |
0.000 |
0.000 |
y |
0.000 |
-25.760 |
0.000 |
z |
0.000 |
0.000 |
-20.918 |
|
Traceless |
| x | y | z |
x |
-0.193 |
0.000 |
0.000 |
y |
0.000 |
-3.535 |
0.000 |
z |
0.000 |
0.000 |
3.728 |
|
Polar |
3z2-r2 | 7.456 |
x2-y2 | 2.228 |
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 |
4.544 |
0.000 |
0.000 |
y |
0.000 |
3.785 |
0.000 |
z |
0.000 |
0.000 |
3.235 |
<r2> (average value of r
2) Å
2
<r2> |
54.630 |
(<r2>)1/2 |
7.391 |