Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.259070 |
| Energy at 298.15K | |
| HF Energy | -1592.259070 |
| Nuclear repulsion energy | 352.014258 |
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 PBE1PBE/aug-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 |
540 |
519 |
0.00 |
39.67 |
0.04 |
0.08 |
| 2 |
A1 |
208 |
200 |
0.00 |
1.06 |
0.72 |
0.84 |
| 3 |
B1 |
479 |
461 |
0.00 |
16.19 |
0.75 |
0.86 |
| 4 |
B2 |
302 |
291 |
0.01 |
6.72 |
0.75 |
0.86 |
| 5 |
E |
453 |
435 |
0.00 |
2.99 |
0.75 |
0.86 |
| 5 |
E |
453 |
435 |
0.00 |
2.99 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1217.2 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1170.4 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 PBE1PBE/aug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.424 |
0.314 |
| S2 |
0.000 |
-1.424 |
0.314 |
| S3 |
-1.424 |
0.000 |
-0.314 |
| S4 |
1.424 |
0.000 |
-0.314 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8477 | 2.1095 | 2.1095 |
S2 | 2.8477 | | 2.1095 | 2.1095 | S3 | 2.1095 | 2.1095 | | 2.8477 | S4 | 2.1095 | 2.1095 | 2.8477 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.548 |
|
S1 |
S3 |
S4 |
47.548 |
| S2 |
S1 |
S3 |
47.548 |
|
S2 |
S4 |
S3 |
47.548 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-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 |
-48.921 |
0.000 |
0.000 |
| y |
0.000 |
-48.921 |
0.000 |
| z |
0.000 |
0.000 |
-54.428 |
|
| Traceless |
| | x | y | z |
| x |
2.753 |
0.000 |
0.000 |
| y |
0.000 |
2.753 |
0.000 |
| z |
0.000 |
0.000 |
-5.507 |
|
| Polar |
| 3z2-r2 | -11.014 |
| 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 |
12.654 |
0.000 |
0.000 |
| y |
0.000 |
12.654 |
0.000 |
| z |
0.000 |
0.000 |
8.958 |
<r2> (average value of r
2) Å
2
| <r2> |
167.780 |
| (<r2>)1/2 |
12.953 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.280230 |
| Energy at 298.15K | |
| HF Energy | -1592.280230 |
| Nuclear repulsion energy | 334.111186 |
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 PBE1PBE/aug-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 |
703 |
676 |
6.96 |
30.72 |
0.06 |
0.11 |
| 2 |
A1 |
409 |
393 |
4.94 |
40.01 |
0.15 |
0.25 |
| 3 |
A1 |
118 |
114 |
0.42 |
10.61 |
0.38 |
0.55 |
| 4 |
A2 |
220 |
212 |
0.00 |
0.16 |
0.75 |
0.86 |
| 5 |
B2 |
674 |
648 |
121.51 |
3.97 |
0.75 |
0.86 |
| 6 |
B2 |
341 |
328 |
0.18 |
7.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1233.1 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1185.6 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 PBE1PBE/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.047 |
0.915 |
| S2 |
0.000 |
-1.047 |
0.915 |
| S3 |
0.000 |
1.584 |
-0.915 |
| S4 |
0.000 |
-1.584 |
-0.915 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0936 | 1.9068 | 3.2044 |
S2 | 2.0936 | | 3.2044 | 1.9068 | S3 | 1.9068 | 3.2044 | | 3.1680 | S4 | 3.2044 | 1.9068 | 3.1680 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.364 |
|
S1 |
S3 |
S4 |
73.636 |
| S2 |
S1 |
S3 |
106.364 |
|
S2 |
S4 |
S3 |
73.636 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.180 |
|
|
|
| 2 |
S |
0.180 |
|
|
|
| 3 |
S |
-0.180 |
|
|
|
| 4 |
S |
-0.180 |
|
|
|
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 |
1.364 |
1.364 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.418 |
0.000 |
0.000 |
| y |
0.000 |
-53.218 |
0.000 |
| z |
0.000 |
0.000 |
-48.567 |
|
| Traceless |
| | x | y | z |
| x |
-0.526 |
0.000 |
0.000 |
| y |
0.000 |
-3.226 |
0.000 |
| z |
0.000 |
0.000 |
3.752 |
|
| Polar |
| 3z2-r2 | 7.504 |
| x2-y2 | 1.800 |
| 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 |
8.177 |
0.000 |
0.000 |
| y |
0.000 |
19.821 |
0.000 |
| z |
0.000 |
0.000 |
13.089 |
<r2> (average value of r
2) Å
2
| <r2> |
200.808 |
| (<r2>)1/2 |
14.171 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.273850 |
| Energy at 298.15K | |
| HF Energy | -1592.273850 |
| Nuclear repulsion energy | 338.443856 |
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 PBE1PBE/aug-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 |
756 |
727 |
0.00 |
37.24 |
0.09 |
0.16 |
| 2 |
Ag |
311 |
299 |
0.00 |
32.28 |
0.17 |
0.30 |
| 3 |
Au |
258 |
248 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
696 |
669 |
124.06 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
161i |
155i |
16.60 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
349 |
335 |
0.00 |
8.54 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1104.2 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1061.7 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 PBE1PBE/aug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.944 |
1.249 |
| S2 |
0.000 |
0.944 |
-1.249 |
| S3 |
0.000 |
-0.944 |
1.249 |
| S4 |
0.000 |
-0.944 |
-1.249 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4986 | 1.8882 | 3.1318 |
S2 | 2.4986 | | 3.1318 | 1.8882 | S3 | 1.8882 | 3.1318 | | 2.4986 | S4 | 3.1318 | 1.8882 | 2.4986 | |
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 PBE1PBE/aug-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 |
-51.637 |
0.000 |
0.000 |
| y |
0.000 |
-47.850 |
0.000 |
| z |
0.000 |
0.000 |
-52.950 |
|
| Traceless |
| | x | y | z |
| x |
-1.237 |
0.000 |
0.000 |
| y |
0.000 |
4.443 |
0.000 |
| z |
0.000 |
0.000 |
-3.206 |
|
| Polar |
| 3z2-r2 | -6.413 |
| x2-y2 | -3.787 |
| 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 |
8.152 |
0.000 |
0.000 |
| y |
0.000 |
13.464 |
0.000 |
| z |
0.000 |
0.000 |
18.791 |
<r2> (average value of r
2) Å
2
| <r2> |
188.664 |
| (<r2>)1/2 |
13.736 |