Jump to
S2C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -151.941851 |
| Energy at 298.15K | |
| HF Energy | -151.941851 |
| Nuclear repulsion energy | 63.418016 |
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 HSEh1PBE/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 |
2150 |
2065 |
0.00 |
58.80 |
0.64 |
0.78 |
| 2 |
Σg |
946 |
909 |
0.00 |
95.97 |
0.42 |
0.60 |
| 3 |
Σu |
1603 |
1539 |
293.53 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
334 |
321 |
0.00 |
14.54 |
0.75 |
0.86 |
| 4 |
Πg |
334 |
321 |
0.00 |
14.54 |
0.75 |
0.86 |
| 5 |
Πu |
165 |
159 |
24.00 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
165 |
159 |
24.00 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2848.8 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 2736.0 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 HSEh1PBE/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.644 |
| C2 |
0.000 |
0.000 |
-0.644 |
| C3 |
0.000 |
0.000 |
1.954 |
| C4 |
0.000 |
0.000 |
-1.954 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2872 | 1.3104 | 2.5976 |
C2 | 1.2872 | | 2.5976 | 1.3104 | C3 | 1.3104 | 2.5976 | | 3.9080 | C4 | 2.5976 | 1.3104 | 3.9080 | |
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 HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.085 |
|
|
|
| 2 |
C |
0.085 |
|
|
|
| 3 |
C |
-0.085 |
|
|
|
| 4 |
C |
-0.085 |
|
|
|
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 |
-21.885 |
0.000 |
0.000 |
| y |
0.000 |
-21.885 |
0.000 |
| z |
0.000 |
0.000 |
-32.758 |
|
| Traceless |
| | x | y | z |
| x |
5.437 |
0.000 |
0.000 |
| y |
0.000 |
5.437 |
0.000 |
| z |
0.000 |
0.000 |
-10.873 |
|
| Polar |
| 3z2-r2 | -21.747 |
| 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 |
3.391 |
0.000 |
0.000 |
| y |
0.000 |
3.391 |
0.000 |
| z |
0.000 |
0.000 |
12.963 |
<r2> (average value of r
2) Å
2
| <r2> |
66.720 |
| (<r2>)1/2 |
8.168 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -151.908840 |
| Energy at 298.15K | |
| HF Energy | -151.908840 |
| Nuclear repulsion energy | 63.320502 |
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 HSEh1PBE/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 |
2152 |
2067 |
0.00 |
69.90 |
0.42 |
0.60 |
| 2 |
Σg |
943 |
905 |
0.00 |
77.79 |
0.34 |
0.51 |
| 3 |
Σu |
1612 |
1548 |
386.34 |
0.00 |
0.00 |
0.00 |
| 4 |
Πg |
464 |
446 |
0.00 |
5.95 |
0.75 |
0.86 |
| 4 |
Πg |
260 |
249 |
0.00 |
11.65 |
0.75 |
0.86 |
| 5 |
Πu |
205 |
197 |
6.39 |
0.00 |
0.00 |
0.00 |
| 5 |
Πu |
140 |
135 |
34.42 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 2887.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 2773.3 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 HSEh1PBE/6-311G**
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.646 |
| C2 |
0.000 |
0.000 |
-0.646 |
| C3 |
0.000 |
0.000 |
1.957 |
| C4 |
0.000 |
0.000 |
-1.957 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
C3 |
C4 |
| C1 | | 1.2918 | 1.3108 | 2.6026 |
C2 | 1.2918 | | 2.6026 | 1.3108 | C3 | 1.3108 | 2.6026 | | 3.9135 | C4 | 2.6026 | 1.3108 | 3.9135 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.083 |
|
|
|
| 2 |
C |
0.083 |
|
|
|
| 3 |
C |
-0.083 |
|
|
|
| 4 |
C |
-0.083 |
|
|
|
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 |
-23.822 |
0.000 |
0.000 |
| y |
0.000 |
-20.126 |
0.000 |
| z |
0.000 |
0.000 |
-32.495 |
|
| Traceless |
| | x | y | z |
| x |
2.488 |
0.000 |
0.000 |
| y |
0.000 |
8.033 |
0.000 |
| z |
0.000 |
0.000 |
-10.521 |
|
| Polar |
| 3z2-r2 | -21.043 |
| x2-y2 | -3.696 |
| 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 |
2.990 |
0.000 |
0.000 |
| y |
0.000 |
3.273 |
0.000 |
| z |
0.000 |
0.000 |
12.478 |
<r2> (average value of r
2) Å
2
| <r2> |
66.867 |
| (<r2>)1/2 |
8.177 |