Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.182500 |
| Energy at 298.15K | |
| HF Energy | -1592.182500 |
| Nuclear repulsion energy | 347.704530 |
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/cc-pVDZ
| 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 |
525 |
505 |
0.00 |
41.28 |
0.05 |
0.10 |
| 2 |
A1 |
197 |
189 |
0.00 |
3.53 |
0.75 |
0.86 |
| 3 |
B1 |
460 |
442 |
0.00 |
23.83 |
0.75 |
0.86 |
| 4 |
B2 |
304 |
293 |
0.08 |
11.30 |
0.75 |
0.86 |
| 5 |
E |
437 |
420 |
0.10 |
5.65 |
0.75 |
0.86 |
| 5 |
E |
437 |
420 |
0.10 |
5.65 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1179.4 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1134.0 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 PBE1PBE/cc-pVDZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.442 |
0.316 |
| S2 |
0.000 |
-1.442 |
0.316 |
| S3 |
-1.442 |
0.000 |
-0.316 |
| S4 |
1.442 |
0.000 |
-0.316 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8842 | 2.1353 | 2.1353 |
S2 | 2.8842 | | 2.1353 | 2.1353 | S3 | 2.1353 | 2.1353 | | 2.8842 | S4 | 2.1353 | 2.1353 | 2.8842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.518 |
|
S1 |
S3 |
S4 |
47.518 |
| S2 |
S1 |
S3 |
47.518 |
|
S2 |
S4 |
S3 |
47.518 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
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 |
-48.918 |
0.000 |
0.000 |
| y |
0.000 |
-48.918 |
0.000 |
| z |
0.000 |
0.000 |
-54.574 |
|
| Traceless |
| | x | y | z |
| x |
2.828 |
0.000 |
0.000 |
| y |
0.000 |
2.828 |
0.000 |
| z |
0.000 |
0.000 |
-5.657 |
|
| Polar |
| 3z2-r2 | -11.314 |
| 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 |
10.256 |
0.000 |
0.000 |
| y |
0.000 |
10.256 |
0.000 |
| z |
0.000 |
0.000 |
5.033 |
<r2> (average value of r
2) Å
2
| <r2> |
171.236 |
| (<r2>)1/2 |
13.086 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.207339 |
| Energy at 298.15K | |
| HF Energy | -1592.207339 |
| Nuclear repulsion energy | 331.394619 |
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/cc-pVDZ
| 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 |
3.21 |
27.58 |
0.22 |
0.36 |
| 2 |
A1 |
360 |
346 |
8.09 |
34.08 |
0.22 |
0.36 |
| 3 |
A1 |
118 |
114 |
1.82 |
8.03 |
0.50 |
0.67 |
| 4 |
A2 |
222 |
213 |
0.00 |
0.08 |
0.75 |
0.86 |
| 5 |
B2 |
675 |
649 |
122.97 |
2.09 |
0.75 |
0.86 |
| 6 |
B2 |
339 |
326 |
0.10 |
15.06 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1208.1 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1161.6 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/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.081 |
0.932 |
| S2 |
0.000 |
-1.081 |
0.932 |
| S3 |
0.000 |
1.549 |
-0.932 |
| S4 |
0.000 |
-1.549 |
-0.932 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1629 | 1.9215 | 3.2240 |
S2 | 2.1629 | | 3.2240 | 1.9215 | S3 | 1.9215 | 3.2240 | | 3.0987 | S4 | 3.2240 | 1.9215 | 3.0987 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
104.094 |
|
S1 |
S3 |
S4 |
75.906 |
| S2 |
S1 |
S3 |
104.094 |
|
S2 |
S4 |
S3 |
75.906 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.096 |
|
|
|
| 2 |
S |
0.096 |
|
|
|
| 3 |
S |
-0.096 |
|
|
|
| 4 |
S |
-0.096 |
|
|
|
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 |
1.357 |
1.357 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.297 |
0.000 |
0.000 |
| y |
0.000 |
-53.303 |
0.000 |
| z |
0.000 |
0.000 |
-48.443 |
|
| Traceless |
| | x | y | z |
| x |
-0.424 |
0.000 |
0.000 |
| y |
0.000 |
-3.433 |
0.000 |
| z |
0.000 |
0.000 |
3.857 |
|
| Polar |
| 3z2-r2 | 7.713 |
| x2-y2 | 2.006 |
| 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 |
4.152 |
0.000 |
0.000 |
| y |
0.000 |
16.552 |
0.000 |
| z |
0.000 |
0.000 |
10.976 |
<r2> (average value of r
2) Å
2
| <r2> |
201.675 |
| (<r2>)1/2 |
14.201 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.204042 |
| Energy at 298.15K | |
| HF Energy | -1592.204042 |
| Nuclear repulsion energy | 333.772747 |
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/cc-pVDZ
| 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 |
746 |
718 |
0.00 |
32.34 |
0.27 |
0.42 |
| 2 |
Ag |
300 |
289 |
0.00 |
33.64 |
0.27 |
0.43 |
| 3 |
Au |
250 |
241 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
692 |
666 |
132.28 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
125i |
121i |
17.00 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
343 |
330 |
0.00 |
16.64 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1103.6 cm
-1
Scaled (by 0.9615) Zero Point Vibrational Energy (zpe) 1061.1 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 PBE1PBE/cc-pVDZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.954 |
1.272 |
| S2 |
0.000 |
0.954 |
-1.272 |
| S3 |
0.000 |
-0.954 |
1.272 |
| S4 |
0.000 |
-0.954 |
-1.272 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5440 | 1.9072 | 3.1796 |
S2 | 2.5440 | | 3.1796 | 1.9072 | S3 | 1.9072 | 3.1796 | | 2.5440 | S4 | 3.1796 | 1.9072 | 2.5440 | |
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/cc-pVDZ
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 |
-51.588 |
0.000 |
0.000 |
| y |
0.000 |
-47.948 |
0.000 |
| z |
0.000 |
0.000 |
-53.035 |
|
| Traceless |
| | x | y | z |
| x |
-1.097 |
0.000 |
0.000 |
| y |
0.000 |
4.364 |
0.000 |
| z |
0.000 |
0.000 |
-3.267 |
|
| Polar |
| 3z2-r2 | -6.535 |
| x2-y2 | -3.640 |
| 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 |
4.126 |
0.000 |
0.000 |
| y |
0.000 |
11.422 |
0.000 |
| z |
0.000 |
0.000 |
15.877 |
<r2> (average value of r
2) Å
2
| <r2> |
193.517 |
| (<r2>)1/2 |
13.911 |