Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/STO-3G
| | hartrees |
| Energy at 0K | -1574.654585 |
| Energy at 298.15K | |
| HF Energy | -1574.654585 |
| Nuclear repulsion energy | 344.780567 |
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/STO-3G
| 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 |
642 |
567 |
0.00 |
24.79 |
0.09 |
0.16 |
| 2 |
A1 |
161 |
143 |
0.00 |
1.76 |
0.73 |
0.84 |
| 3 |
B1 |
586 |
517 |
0.00 |
15.44 |
0.75 |
0.86 |
| 4 |
B2 |
346 |
305 |
0.99 |
6.08 |
0.75 |
0.86 |
| 5 |
E |
573 |
506 |
1.57 |
3.48 |
0.75 |
0.86 |
| 5 |
E |
573 |
506 |
1.57 |
3.48 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1440.6 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 1272.2 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/STO-3G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.472 |
0.257 |
| S2 |
0.000 |
-1.472 |
0.257 |
| S3 |
-1.472 |
0.000 |
-0.257 |
| S4 |
1.472 |
0.000 |
-0.257 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9437 | 2.1440 | 2.1440 |
S2 | 2.9437 | | 2.1440 | 2.1440 | S3 | 2.1440 | 2.1440 | | 2.9437 | S4 | 2.1440 | 2.1440 | 2.9437 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
46.646 |
|
S1 |
S3 |
S4 |
46.646 |
| S2 |
S1 |
S3 |
46.646 |
|
S2 |
S4 |
S3 |
46.646 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
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 |
-43.846 |
0.000 |
0.000 |
| y |
0.000 |
-43.846 |
0.000 |
| z |
0.000 |
0.000 |
-45.789 |
|
| Traceless |
| | x | y | z |
| x |
0.972 |
0.000 |
0.000 |
| y |
0.000 |
0.972 |
0.000 |
| z |
0.000 |
0.000 |
-1.944 |
|
| Polar |
| 3z2-r2 | -3.887 |
| 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 |
5.825 |
0.000 |
0.000 |
| y |
0.000 |
5.825 |
0.000 |
| z |
0.000 |
0.000 |
0.897 |
<r2> (average value of r
2) Å
2
| <r2> |
170.662 |
| (<r2>)1/2 |
13.064 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/STO-3G
| | hartrees |
| Energy at 0K | -1574.621109 |
| Energy at 298.15K | |
| HF Energy | -1574.621109 |
| Nuclear repulsion energy | 329.753216 |
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/STO-3G
| 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 |
774 |
684 |
0.02 |
15.28 |
0.20 |
0.33 |
| 2 |
A1 |
395 |
349 |
6.13 |
13.98 |
0.23 |
0.38 |
| 3 |
A1 |
133 |
118 |
5.33 |
3.12 |
0.53 |
0.69 |
| 4 |
A2 |
207 |
183 |
0.00 |
0.02 |
0.75 |
0.86 |
| 5 |
B2 |
776 |
686 |
30.76 |
0.55 |
0.75 |
0.86 |
| 6 |
B2 |
340 |
301 |
0.46 |
8.73 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1313.2 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 1159.7 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 HSEh1PBE/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.129 |
0.963 |
| S2 |
0.000 |
-1.129 |
0.963 |
| S3 |
0.000 |
1.448 |
-0.963 |
| S4 |
0.000 |
-1.448 |
-0.963 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.2579 | 1.9527 | 3.2172 |
S2 | 2.2579 | | 3.2172 | 1.9527 | S3 | 1.9527 | 3.2172 | | 2.8953 | S4 | 3.2172 | 1.9527 | 2.8953 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
99.393 |
|
S1 |
S3 |
S4 |
80.607 |
| S2 |
S1 |
S3 |
99.393 |
|
S2 |
S4 |
S3 |
80.607 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.055 |
|
|
|
| 2 |
S |
0.055 |
|
|
|
| 3 |
S |
-0.055 |
|
|
|
| 4 |
S |
-0.055 |
|
|
|
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 |
1.066 |
1.066 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-42.423 |
0.000 |
0.000 |
| y |
0.000 |
-45.048 |
0.000 |
| z |
0.000 |
0.000 |
-44.736 |
|
| Traceless |
| | x | y | z |
| x |
2.469 |
0.000 |
0.000 |
| y |
0.000 |
-1.469 |
0.000 |
| z |
0.000 |
0.000 |
-1.000 |
|
| Polar |
| 3z2-r2 | -2.001 |
| x2-y2 | 2.625 |
| 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 |
1.209 |
0.000 |
0.000 |
| y |
0.000 |
9.359 |
0.000 |
| z |
0.000 |
0.000 |
6.329 |
<r2> (average value of r
2) Å
2
| <r2> |
194.755 |
| (<r2>)1/2 |
13.955 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/STO-3G
| | hartrees |
| Energy at 0K | -1574.619625 |
| Energy at 298.15K | |
| HF Energy | -1574.619625 |
| Nuclear repulsion energy | 331.639611 |
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/STO-3G
| 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 |
819 |
723 |
0.00 |
15.62 |
0.23 |
0.37 |
| 2 |
Ag |
377 |
333 |
0.00 |
16.30 |
0.26 |
0.41 |
| 3 |
Au |
231 |
204 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
802 |
708 |
36.66 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
122i |
108i |
20.14 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
347 |
306 |
0.00 |
9.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1226.9 cm
-1
Scaled (by 0.8831) Zero Point Vibrational Energy (zpe) 1083.5 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/STO-3G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.970 |
1.266 |
| S2 |
0.000 |
0.970 |
-1.266 |
| S3 |
0.000 |
-0.970 |
1.266 |
| S4 |
0.000 |
-0.970 |
-1.266 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5326 | 1.9392 | 3.1898 |
S2 | 2.5326 | | 3.1898 | 1.9392 | S3 | 1.9392 | 3.1898 | | 2.5326 | S4 | 3.1898 | 1.9392 | 2.5326 | |
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/STO-3G
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 |
-42.428 |
0.000 |
0.000 |
| y |
0.000 |
-44.647 |
0.000 |
| z |
0.000 |
0.000 |
-44.259 |
|
| Traceless |
| | x | y | z |
| x |
2.025 |
0.000 |
0.000 |
| y |
0.000 |
-1.303 |
0.000 |
| z |
0.000 |
0.000 |
-0.722 |
|
| Polar |
| 3z2-r2 | -1.444 |
| x2-y2 | 2.218 |
| 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 |
1.192 |
0.000 |
0.000 |
| y |
0.000 |
6.523 |
0.000 |
| z |
0.000 |
0.000 |
9.019 |
<r2> (average value of r
2) Å
2
| <r2> |
190.136 |
| (<r2>)1/2 |
13.789 |