Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G(2df,p)
| hartrees |
Energy at 0K | -1194.157628 |
Energy at 298.15K | -1194.158083 |
HF Energy | -1194.157628 |
Nuclear repulsion energy | 182.773189 |
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 HSEh1PBE/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.657 |
S2 |
0.000 |
1.642 |
-0.328 |
S3 |
0.000 |
-1.642 |
-0.328 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
S1 | | 1.9146 | 1.9146 |
S2 | 1.9146 | | 3.2834 | S3 | 1.9146 | 3.2834 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S2 |
S1 |
S3 |
118.070 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.241 |
|
|
|
2 |
S |
-0.120 |
|
|
|
3 |
S |
-0.120 |
|
|
|
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 |
0.575 |
0.575 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.004 |
0.000 |
0.000 |
y |
0.000 |
-38.668 |
0.000 |
z |
0.000 |
0.000 |
-38.797 |
|
Traceless |
| x | y | z |
x |
1.729 |
0.000 |
0.000 |
y |
0.000 |
-0.768 |
0.000 |
z |
0.000 |
0.000 |
-0.961 |
|
Polar |
3z2-r2 | -1.922 |
x2-y2 | 1.665 |
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 |
4.489 |
0.000 |
0.000 |
y |
0.000 |
14.641 |
0.000 |
z |
0.000 |
0.000 |
5.908 |
<r2> (average value of r
2) Å
2
<r2> |
120.429 |
(<r2>)1/2 |
10.974 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G(2df,p)
| hartrees |
Energy at 0K | -1194.151721 |
Energy at 298.15K | -1194.152277 |
HF Energy | -1194.151721 |
Nuclear repulsion energy | 196.184591 |
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 HSEh1PBE/6-31G(2df,p)
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
1.196 |
0.000 |
S2 |
1.036 |
-0.598 |
0.000 |
S3 |
-1.036 |
-0.598 |
0.000 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
S1 | | 2.0716 | 2.0716 |
S2 | 2.0716 | | 2.0716 | S3 | 2.0716 | 2.0716 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S2 |
S1 |
S3 |
60.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
0.000 |
|
|
|
2 |
S |
0.000 |
|
|
|
3 |
S |
0.000 |
|
|
|
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 |
-35.243 |
0.000 |
0.000 |
y |
0.000 |
-35.243 |
0.000 |
z |
0.000 |
0.000 |
-41.518 |
|
Traceless |
| x | y | z |
x |
3.138 |
0.000 |
0.000 |
y |
0.000 |
3.138 |
0.000 |
z |
0.000 |
0.000 |
-6.275 |
|
Polar |
3z2-r2 | -12.551 |
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 |
8.116 |
0.000 |
0.000 |
y |
0.000 |
8.116 |
0.000 |
z |
0.000 |
0.000 |
4.705 |
<r2> (average value of r
2) Å
2
<r2> |
91.980 |
(<r2>)1/2 |
9.591 |