Jump to
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -551.532317 |
| Energy at 298.15K | |
| HF Energy | -551.532317 |
| Nuclear repulsion energy | 355.502030 |
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 B1B95/6-311G*
Geometric Data calculated at B1B95/6-311G*
Point Group is D4h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
1.009 |
0.000 |
| C2 |
1.009 |
0.000 |
0.000 |
| C3 |
0.000 |
-1.009 |
0.000 |
| C4 |
-1.009 |
0.000 |
0.000 |
| F5 |
0.000 |
2.316 |
0.000 |
| F6 |
2.316 |
0.000 |
0.000 |
| F7 |
0.000 |
-2.316 |
0.000 |
| F8 |
-2.316 |
0.000 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
| C1 | | 1.4275 | 2.0188 | 1.4275 | 1.3062 | 2.5261 | 3.3250 | 2.5261 |
C2 | 1.4275 | | 1.4275 | 2.0188 | 2.5261 | 1.3062 | 2.5261 | 3.3250 | C3 | 2.0188 | 1.4275 | | 1.4275 | 3.3250 | 2.5261 | 1.3062 | 2.5261 | C4 | 1.4275 | 2.0188 | 1.4275 | | 2.5261 | 3.3250 | 2.5261 | 1.3062 | F5 | 1.3062 | 2.5261 | 3.3250 | 2.5261 | | 3.2748 | 4.6312 | 3.2748 | F6 | 2.5261 | 1.3062 | 2.5261 | 3.3250 | 3.2748 | | 3.2748 | 4.6312 | F7 | 3.3250 | 2.5261 | 1.3062 | 2.5261 | 4.6312 | 3.2748 | | 3.2748 | F8 | 2.5261 | 3.3250 | 2.5261 | 1.3062 | 3.2748 | 4.6312 | 3.2748 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
90.000 |
|
C1 |
C2 |
F6 |
135.000 |
| C1 |
C4 |
C3 |
90.000 |
|
C1 |
C4 |
F8 |
135.000 |
| C2 |
C1 |
C4 |
90.000 |
|
C2 |
C1 |
F5 |
135.000 |
| C2 |
C3 |
C4 |
90.000 |
|
C2 |
C3 |
F7 |
135.000 |
| C3 |
C2 |
F6 |
135.000 |
|
C3 |
C4 |
F8 |
135.000 |
| C4 |
C1 |
F5 |
135.000 |
|
C4 |
C3 |
F7 |
135.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.362 |
|
|
|
| 2 |
C |
-0.052 |
|
|
|
| 3 |
C |
0.362 |
|
|
|
| 4 |
C |
-0.052 |
|
|
|
| 5 |
F |
-0.116 |
|
|
|
| 6 |
F |
-0.195 |
|
|
|
| 7 |
F |
-0.116 |
|
|
|
| 8 |
F |
-0.195 |
|
|
|
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 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.349 |
0.000 |
0.000 |
| y |
0.000 |
-37.850 |
0.000 |
| z |
0.000 |
0.000 |
-40.424 |
|
| Traceless |
| | x | y | z |
| x |
-9.211 |
0.000 |
0.000 |
| y |
0.000 |
6.536 |
0.000 |
| z |
0.000 |
0.000 |
2.675 |
|
| Polar |
| 3z2-r2 | 5.350 |
| x2-y2 | -10.499 |
| 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 |
6.946 |
0.000 |
0.000 |
| y |
0.000 |
7.519 |
0.000 |
| z |
0.000 |
0.000 |
3.217 |
<r2> (average value of r
2) Å
2
| <r2> |
243.850 |
| (<r2>)1/2 |
15.616 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -551.611856 |
| Energy at 298.15K | -551.611845 |
| HF Energy | -551.611856 |
| Nuclear repulsion energy | 356.077087 |
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 B1B95/6-311G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
1897 |
1818 |
0.00 |
|
|
|
| 2 |
Ag |
1247 |
1195 |
0.00 |
|
|
|
| 3 |
Ag |
712 |
683 |
0.00 |
|
|
|
| 4 |
Ag |
298 |
286 |
0.00 |
|
|
|
| 5 |
Ag |
174 |
167 |
0.00 |
|
|
|
| 6 |
Au |
1338 |
1282 |
559.72 |
|
|
|
| 7 |
Au |
943 |
904 |
54.72 |
|
|
|
| 8 |
Au |
612 |
587 |
56.80 |
|
|
|
| 9 |
Au |
241 |
231 |
0.08 |
|
|
|
| 10 |
Au |
157 |
150 |
0.03 |
|
|
|
| 11 |
Bg |
1363 |
1307 |
0.00 |
|
|
|
| 12 |
Bg |
771 |
739 |
0.00 |
|
|
|
| 13 |
Bg |
493 |
473 |
0.00 |
|
|
|
| 14 |
Bg |
406 |
389 |
0.00 |
|
|
|
| 15 |
Bu |
1870 |
1792 |
201.43 |
|
|
|
| 16 |
Bu |
1002 |
960 |
212.41 |
|
|
|
| 17 |
Bu |
313 |
300 |
6.00 |
|
|
|
| 18 |
Bu |
188 |
180 |
2.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7011.3 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 6721.0 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 B1B95/6-311G*
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.108 |
0.767 |
0.661 |
| C2 |
-0.108 |
-0.767 |
0.661 |
| C3 |
-0.108 |
-0.767 |
-0.661 |
| C4 |
0.108 |
0.767 |
-0.661 |
| F5 |
-0.108 |
1.652 |
1.602 |
| F6 |
0.108 |
-1.652 |
1.602 |
| F7 |
0.108 |
-1.652 |
-1.602 |
| F8 |
-0.108 |
1.652 |
-1.602 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
F5 |
F6 |
F7 |
F8 |
| C1 | | 1.5488 | 2.0360 | 1.3216 | 1.3099 | 2.5953 | 3.3120 | 2.4392 |
C2 | 1.5488 | | 1.3216 | 2.0360 | 2.5953 | 1.3099 | 2.4392 | 3.3120 | C3 | 2.0360 | 1.3216 | | 1.5488 | 3.3120 | 2.4392 | 1.3099 | 2.5953 | C4 | 1.3216 | 2.0360 | 1.5488 | | 2.4392 | 3.3120 | 2.5953 | 1.3099 | F5 | 1.3099 | 2.5953 | 3.3120 | 2.4392 | | 3.3109 | 4.6071 | 3.2036 | F6 | 2.5953 | 1.3099 | 2.4392 | 3.3120 | 3.3109 | | 3.2036 | 4.6071 | F7 | 3.3120 | 2.4392 | 1.3099 | 2.5953 | 4.6071 | 3.2036 | | 3.3109 | F8 | 2.4392 | 3.3120 | 2.5953 | 1.3099 | 3.2036 | 4.6071 | 3.3109 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C3 |
90.000 |
|
C1 |
C2 |
F6 |
130.238 |
| C1 |
C4 |
C3 |
90.000 |
|
C1 |
C4 |
F8 |
135.924 |
| C2 |
C1 |
C4 |
90.000 |
|
C2 |
C1 |
F5 |
130.238 |
| C2 |
C3 |
C4 |
90.000 |
|
C2 |
C3 |
F7 |
135.924 |
| C3 |
C2 |
F6 |
135.924 |
|
C3 |
C4 |
F8 |
130.238 |
| C4 |
C1 |
F5 |
135.924 |
|
C4 |
C3 |
F7 |
130.238 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.164 |
|
|
|
| 2 |
C |
0.164 |
|
|
|
| 3 |
C |
0.164 |
|
|
|
| 4 |
C |
0.164 |
|
|
|
| 5 |
F |
-0.164 |
|
|
|
| 6 |
F |
-0.164 |
|
|
|
| 7 |
F |
-0.164 |
|
|
|
| 8 |
F |
-0.164 |
|
|
|
Electric dipole moments
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-40.124 |
-0.035 |
0.000 |
| y |
-0.035 |
-43.567 |
0.000 |
| z |
0.000 |
0.000 |
-43.169 |
|
| Traceless |
| | x | y | z |
| x |
3.244 |
-0.035 |
0.000 |
| y |
-0.035 |
-1.921 |
0.000 |
| z |
0.000 |
0.000 |
-1.323 |
|
| Polar |
| 3z2-r2 | -2.646 |
| x2-y2 | 3.443 |
| xy | -0.035 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.148 |
-0.005 |
0.000 |
| y |
-0.005 |
5.831 |
0.000 |
| z |
0.000 |
0.000 |
7.446 |
<r2> (average value of r
2) Å
2
| <r2> |
242.312 |
| (<r2>)1/2 |
15.566 |