Jump to
S2C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -152.056490 |
| Energy at 298.15K | |
| HF Energy | -152.056490 |
| Nuclear repulsion energy | 63.511045 |
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 |
Σg |
2155 |
2066 |
0.00 |
58.37 |
0.55 |
0.71 |
| 2 |
Σg |
947 |
908 |
0.00 |
91.77 |
0.39 |
0.56 |
| 3 |
Σu |
1610 |
1543 |
309.38 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
353 |
339 |
0.00 |
4.83 |
0.75 |
0.86 |
| 4 |
Πg |
353 |
339 |
0.00 |
4.83 |
0.75 |
0.86 |
| 5 |
Πu |
167 |
160 |
21.81 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
167 |
160 |
21.81 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2876.4 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 2757.3 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 B1B95/6-311G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.643 |
| C2 |
0.000 |
0.000 |
-0.643 |
| C3 |
0.000 |
0.000 |
1.951 |
| C4 |
0.000 |
0.000 |
-1.951 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2870 | 1.3075 | 2.5944 |
C2 | 1.2870 | | 2.5944 | 1.3075 | C3 | 1.3075 | 2.5944 | | 3.9019 | C4 | 2.5944 | 1.3075 | 3.9019 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
C4 |
180.000 |
|
C2 |
C1 |
C3 |
180.000 |
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 |
0.079 |
|
|
|
| 2 |
C |
0.079 |
|
|
|
| 3 |
C |
-0.079 |
|
|
|
| 4 |
C |
-0.079 |
|
|
|
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 |
-21.789 |
0.000 |
0.000 |
| y |
0.000 |
-21.789 |
0.000 |
| z |
0.000 |
0.000 |
-32.467 |
|
| Traceless |
| | x | y | z |
| x |
5.339 |
0.000 |
0.000 |
| y |
0.000 |
5.339 |
0.000 |
| z |
0.000 |
0.000 |
-10.678 |
|
| Polar |
| 3z2-r2 | -21.356 |
| x2-y2 | 0.000 |
| 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 |
3.277 |
0.000 |
0.000 |
| y |
0.000 |
3.277 |
0.000 |
| z |
0.000 |
0.000 |
12.784 |
<r2> (average value of r
2) Å
2
| <r2> |
66.476 |
| (<r2>)1/2 |
8.153 |
Jump to
S1C1
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -152.026212 |
| Energy at 298.15K | |
| HF Energy | -152.026212 |
| Nuclear repulsion energy | 63.411541 |
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 |
Σg |
2158 |
2068 |
0.00 |
71.62 |
0.41 |
0.59 |
| 2 |
Σg |
943 |
904 |
0.00 |
77.00 |
0.34 |
0.50 |
| 3 |
Σu |
1615 |
1549 |
391.41 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
461 |
442 |
0.00 |
6.17 |
0.75 |
0.86 |
| 4 |
Πg |
265 |
254 |
0.00 |
10.09 |
0.75 |
0.86 |
| 5 |
Πu |
204 |
196 |
6.12 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
138 |
133 |
33.62 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2892.4 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 2772.7 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 B1B95/6-311G*
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.645 |
| C2 |
0.000 |
0.000 |
-0.645 |
| C3 |
0.000 |
0.000 |
1.954 |
| C4 |
0.000 |
0.000 |
-1.954 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2908 | 1.3085 | 2.5992 |
C2 | 1.2908 | | 2.5992 | 1.3085 | C3 | 1.3085 | 2.5992 | | 3.9077 | C4 | 2.5992 | 1.3085 | 3.9077 | |
More geometry information
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 |
0.078 |
|
|
|
| 2 |
C |
0.078 |
|
|
|
| 3 |
C |
-0.078 |
|
|
|
| 4 |
C |
-0.078 |
|
|
|
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 |
-20.045 |
0.000 |
0.000 |
| y |
0.000 |
-23.701 |
0.000 |
| z |
0.000 |
0.000 |
-32.250 |
|
| Traceless |
| | x | y | z |
| x |
7.931 |
0.000 |
0.000 |
| y |
0.000 |
2.446 |
0.000 |
| z |
0.000 |
0.000 |
-10.377 |
|
| Polar |
| 3z2-r2 | -20.754 |
| x2-y2 | 3.656 |
| 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 |
3.232 |
0.000 |
0.000 |
| y |
0.000 |
2.967 |
0.000 |
| z |
0.000 |
0.000 |
12.397 |
<r2> (average value of r
2) Å
2
| <r2> |
66.630 |
| (<r2>)1/2 |
8.163 |