Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.256249 |
| Energy at 298.15K | |
| HF Energy | -1592.256249 |
| Nuclear repulsion energy | 352.045405 |
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-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 |
541 |
520 |
0.00 |
39.30 |
0.04 |
0.08 |
| 2 |
A1 |
207 |
199 |
0.00 |
2.32 |
0.75 |
0.85 |
| 3 |
B1 |
480 |
461 |
0.00 |
17.03 |
0.75 |
0.86 |
| 4 |
B2 |
302 |
291 |
0.00 |
8.39 |
0.75 |
0.86 |
| 5 |
E |
453 |
435 |
0.00 |
4.23 |
0.75 |
0.86 |
| 5 |
E |
453 |
435 |
0.00 |
4.23 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1217.9 cm
-1
Scaled (by 0.961) 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/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 | | 2.8475 | 2.1093 | 2.1093 |
S2 | 2.8475 | | 2.1093 | 2.1093 | S3 | 2.1093 | 2.1093 | | 2.8475 | S4 | 2.1093 | 2.1093 | 2.8475 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.549 |
|
S1 |
S3 |
S4 |
47.549 |
| S2 |
S1 |
S3 |
47.549 |
|
S2 |
S4 |
S3 |
47.549 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/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 |
-48.664 |
0.000 |
0.000 |
| y |
0.000 |
-48.664 |
0.000 |
| z |
0.000 |
0.000 |
-54.110 |
|
| Traceless |
| | x | y | z |
| x |
2.723 |
0.000 |
0.000 |
| y |
0.000 |
2.723 |
0.000 |
| z |
0.000 |
0.000 |
-5.446 |
|
| Polar |
| 3z2-r2 | -10.892 |
| 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 |
11.283 |
0.000 |
0.000 |
| y |
0.000 |
11.283 |
0.000 |
| z |
0.000 |
0.000 |
6.635 |
<r2> (average value of r
2) Å
2
| <r2> |
167.581 |
| (<r2>)1/2 |
12.945 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.277818 |
| Energy at 298.15K | |
| HF Energy | -1592.277818 |
| Nuclear repulsion energy | 334.197028 |
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-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 |
705 |
677 |
6.24 |
26.44 |
0.15 |
0.26 |
| 2 |
A1 |
408 |
392 |
5.84 |
39.51 |
0.19 |
0.32 |
| 3 |
A1 |
119 |
114 |
0.52 |
10.42 |
0.44 |
0.61 |
| 4 |
A2 |
222 |
213 |
0.00 |
0.12 |
0.75 |
0.86 |
| 5 |
B2 |
676 |
650 |
121.80 |
3.50 |
0.75 |
0.86 |
| 6 |
B2 |
342 |
329 |
0.20 |
11.46 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1235.5 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 1187.4 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/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.048 |
0.915 |
| S2 |
0.000 |
-1.048 |
0.915 |
| S3 |
0.000 |
1.581 |
-0.915 |
| S4 |
0.000 |
-1.581 |
-0.915 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0952 | 1.9068 | 3.2029 |
S2 | 2.0952 | | 3.2029 | 1.9068 | S3 | 1.9068 | 3.2029 | | 3.1610 | S4 | 3.2029 | 1.9068 | 3.1610 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.229 |
|
S1 |
S3 |
S4 |
73.771 |
| S2 |
S1 |
S3 |
106.229 |
|
S2 |
S4 |
S3 |
73.771 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.135 |
|
|
|
| 2 |
S |
0.135 |
|
|
|
| 3 |
S |
-0.135 |
|
|
|
| 4 |
S |
-0.135 |
|
|
|
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 |
1.448 |
1.448 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.078 |
0.000 |
0.000 |
| y |
0.000 |
-53.092 |
0.000 |
| z |
0.000 |
0.000 |
-48.319 |
|
| Traceless |
| | x | y | z |
| x |
-0.372 |
0.000 |
0.000 |
| y |
0.000 |
-3.393 |
0.000 |
| z |
0.000 |
0.000 |
3.765 |
|
| Polar |
| 3z2-r2 | 7.530 |
| x2-y2 | 2.014 |
| 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 |
5.813 |
0.000 |
0.000 |
| y |
0.000 |
18.132 |
0.000 |
| z |
0.000 |
0.000 |
11.828 |
<r2> (average value of r
2) Å
2
| <r2> |
200.431 |
| (<r2>)1/2 |
14.157 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.271569 |
| Energy at 298.15K | |
| HF Energy | -1592.271569 |
| Nuclear repulsion energy | 338.401246 |
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-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 |
758 |
728 |
0.00 |
33.46 |
0.20 |
0.33 |
| 2 |
Ag |
311 |
299 |
0.00 |
36.82 |
0.24 |
0.39 |
| 3 |
Au |
259 |
249 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
698 |
671 |
126.63 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
160i |
154i |
18.73 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
349 |
336 |
0.00 |
13.04 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1107.0 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 1063.8 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-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.944 |
1.250 |
| S2 |
0.000 |
0.944 |
-1.250 |
| S3 |
0.000 |
-0.944 |
1.250 |
| S4 |
0.000 |
-0.944 |
-1.250 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4992 | 1.8882 | 3.1323 |
S2 | 2.4992 | | 3.1323 | 1.8882 | S3 | 1.8882 | 3.1323 | | 2.4992 | S4 | 3.1323 | 1.8882 | 2.4992 | |
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-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 |
-51.399 |
0.000 |
0.000 |
| y |
0.000 |
-47.661 |
0.000 |
| z |
0.000 |
0.000 |
-52.681 |
|
| Traceless |
| | x | y | z |
| x |
-1.228 |
0.000 |
0.000 |
| y |
0.000 |
4.378 |
0.000 |
| z |
0.000 |
0.000 |
-3.151 |
|
| Polar |
| 3z2-r2 | -6.301 |
| x2-y2 | -3.737 |
| 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 |
5.790 |
0.000 |
0.000 |
| y |
0.000 |
12.316 |
0.000 |
| z |
0.000 |
0.000 |
17.139 |
<r2> (average value of r
2) Å
2
| <r2> |
188.572 |
| (<r2>)1/2 |
13.732 |