Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.325787 |
| Energy at 298.15K | |
| HF Energy | -1592.325787 |
| Nuclear repulsion energy | 351.646784 |
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/daug-cc-pVTZ
| 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 |
536 |
536 |
0.00 |
39.67 |
0.04 |
0.08 |
| 2 |
A1 |
207 |
207 |
0.00 |
1.12 |
0.73 |
0.84 |
| 3 |
B1 |
475 |
475 |
0.00 |
16.02 |
0.75 |
0.86 |
| 4 |
B2 |
302 |
302 |
0.01 |
6.73 |
0.75 |
0.86 |
| 5 |
E |
448 |
448 |
0.00 |
2.96 |
0.75 |
0.86 |
| 5 |
E |
448 |
448 |
0.00 |
2.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1207.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1207.4 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/daug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.425 |
0.315 |
| S2 |
0.000 |
-1.425 |
0.315 |
| S3 |
-1.425 |
0.000 |
-0.315 |
| S4 |
1.425 |
0.000 |
-0.315 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8508 | 2.1117 | 2.1117 |
S2 | 2.8508 | | 2.1117 | 2.1117 | S3 | 2.1117 | 2.1117 | | 2.8508 | S4 | 2.1117 | 2.1117 | 2.8508 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.545 |
|
S1 |
S3 |
S4 |
47.545 |
| S2 |
S1 |
S3 |
47.545 |
|
S2 |
S4 |
S3 |
47.545 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
S |
0.000 |
|
|
|
| 3 |
S |
0.000 |
|
|
|
| 4 |
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 |
-48.963 |
0.000 |
0.000 |
| y |
0.000 |
-48.963 |
0.000 |
| z |
0.000 |
0.000 |
-54.386 |
|
| Traceless |
| | x | y | z |
| x |
2.711 |
0.000 |
0.000 |
| y |
0.000 |
2.711 |
0.000 |
| z |
0.000 |
0.000 |
-5.423 |
|
| Polar |
| 3z2-r2 | -10.846 |
| 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 |
12.777 |
0.000 |
0.000 |
| y |
0.000 |
12.777 |
0.000 |
| z |
0.000 |
0.000 |
9.054 |
<r2> (average value of r
2) Å
2
| <r2> |
168.076 |
| (<r2>)1/2 |
12.964 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.348878 |
| Energy at 298.15K | |
| HF Energy | -1592.348878 |
| Nuclear repulsion energy | 333.436219 |
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/daug-cc-pVTZ
| 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 |
700 |
700 |
6.80 |
30.50 |
0.06 |
0.11 |
| 2 |
A1 |
401 |
401 |
4.87 |
39.40 |
0.14 |
0.25 |
| 3 |
A1 |
117 |
117 |
0.38 |
10.51 |
0.38 |
0.55 |
| 4 |
A2 |
219 |
219 |
0.00 |
0.13 |
0.75 |
0.86 |
| 5 |
B2 |
671 |
671 |
120.29 |
3.89 |
0.75 |
0.86 |
| 6 |
B2 |
340 |
340 |
0.16 |
7.83 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1224.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1224.1 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/daug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.050 |
0.915 |
| S2 |
0.000 |
-1.050 |
0.915 |
| S3 |
0.000 |
1.592 |
-0.915 |
| S4 |
0.000 |
-1.592 |
-0.915 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0990 | 1.9078 | 3.2128 |
S2 | 2.0990 | | 3.2128 | 1.9078 | S3 | 1.9078 | 3.2128 | | 3.1837 | S4 | 3.2128 | 1.9078 | 3.1837 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.515 |
|
S1 |
S3 |
S4 |
73.485 |
| S2 |
S1 |
S3 |
106.515 |
|
S2 |
S4 |
S3 |
73.485 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.324 |
|
|
|
| 2 |
S |
0.324 |
|
|
|
| 3 |
S |
-0.324 |
|
|
|
| 4 |
S |
-0.324 |
|
|
|
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 |
1.348 |
1.348 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.391 |
0.000 |
0.000 |
| y |
0.000 |
-53.236 |
0.000 |
| z |
0.000 |
0.000 |
-48.642 |
|
| Traceless |
| | x | y | z |
| x |
-0.452 |
0.000 |
0.000 |
| y |
0.000 |
-3.220 |
0.000 |
| z |
0.000 |
0.000 |
3.672 |
|
| Polar |
| 3z2-r2 | 7.344 |
| x2-y2 | 1.846 |
| 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 |
8.265 |
0.000 |
0.000 |
| y |
0.000 |
19.938 |
0.000 |
| z |
0.000 |
0.000 |
13.208 |
<r2> (average value of r
2) Å
2
| <r2> |
201.773 |
| (<r2>)1/2 |
14.205 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.342501 |
| Energy at 298.15K | |
| HF Energy | -1592.342501 |
| Nuclear repulsion energy | 337.594797 |
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/daug-cc-pVTZ
| 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 |
752 |
752 |
0.00 |
36.44 |
0.09 |
0.16 |
| 2 |
Ag |
304 |
304 |
0.00 |
32.12 |
0.17 |
0.29 |
| 3 |
Au |
256 |
256 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
693 |
693 |
123.29 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
160i |
160i |
15.88 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
346 |
346 |
0.00 |
8.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1095.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1095.5 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/daug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.945 |
1.255 |
| S2 |
0.000 |
0.945 |
-1.255 |
| S3 |
0.000 |
-0.945 |
1.255 |
| S4 |
0.000 |
-0.945 |
-1.255 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5096 | 1.8896 | 3.1414 |
S2 | 2.5096 | | 3.1414 | 1.8896 | S3 | 1.8896 | 3.1414 | | 2.5096 | S4 | 3.1414 | 1.8896 | 2.5096 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.000 |
|
S1 |
S3 |
S4 |
90.000 |
| S2 |
S1 |
S3 |
90.000 |
|
S2 |
S4 |
S3 |
90.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.000 |
|
|
|
| 2 |
S |
0.000 |
|
|
|
| 3 |
S |
0.000 |
|
|
|
| 4 |
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 |
-51.611 |
0.000 |
0.000 |
| y |
0.000 |
-47.914 |
0.000 |
| z |
0.000 |
0.000 |
-52.975 |
|
| Traceless |
| | x | y | z |
| x |
-1.166 |
0.000 |
0.000 |
| y |
0.000 |
4.379 |
0.000 |
| z |
0.000 |
0.000 |
-3.213 |
|
| Polar |
| 3z2-r2 | -6.426 |
| x2-y2 | -3.697 |
| 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 |
8.235 |
0.000 |
0.000 |
| y |
0.000 |
13.601 |
0.000 |
| z |
0.000 |
0.000 |
18.918 |
<r2> (average value of r
2) Å
2
| <r2> |
189.645 |
| (<r2>)1/2 |
13.771 |