Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.272498 |
| Energy at 298.15K | |
| HF Energy | -1592.272498 |
| Nuclear repulsion energy | 353.670711 |
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-pCVTZ
| 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 |
544 |
544 |
0.00 |
|
|
|
| 2 |
A1 |
210 |
210 |
0.00 |
|
|
|
| 3 |
B1 |
484 |
484 |
0.00 |
|
|
|
| 4 |
B2 |
302 |
302 |
0.00 |
|
|
|
| 5 |
E |
456 |
456 |
0.00 |
|
|
|
| 5 |
E |
456 |
456 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1225.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1225.8 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-pCVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.417 |
0.313 |
| S2 |
0.000 |
-1.417 |
0.313 |
| S3 |
-1.417 |
0.000 |
-0.313 |
| S4 |
1.417 |
0.000 |
-0.313 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8345 | 2.0996 | 2.0996 |
S2 | 2.8345 | | 2.0996 | 2.0996 | S3 | 2.0996 | 2.0996 | | 2.8345 | S4 | 2.0996 | 2.0996 | 2.8345 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.547 |
|
S1 |
S3 |
S4 |
47.547 |
| S2 |
S1 |
S3 |
47.547 |
|
S2 |
S4 |
S3 |
47.547 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pCVTZ
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 |
-48.558 |
0.000 |
0.000 |
| y |
0.000 |
-48.558 |
0.000 |
| z |
0.000 |
0.000 |
-53.982 |
|
| Traceless |
| | x | y | z |
| x |
2.712 |
0.000 |
0.000 |
| y |
0.000 |
2.712 |
0.000 |
| z |
0.000 |
0.000 |
-5.423 |
|
| Polar |
| 3z2-r2 | -10.847 |
| 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 |
11.234 |
0.000 |
0.000 |
| y |
0.000 |
11.234 |
0.000 |
| z |
0.000 |
0.000 |
6.738 |
<r2> (average value of r
2) Å
2
| <r2> |
166.266 |
| (<r2>)1/2 |
12.894 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.295592 |
| Energy at 298.15K | |
| HF Energy | -1592.295592 |
| Nuclear repulsion energy | 335.337953 |
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-pCVTZ
| 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 |
711 |
711 |
7.56 |
|
|
|
| 2 |
A1 |
421 |
421 |
4.79 |
|
|
|
| 3 |
A1 |
117 |
117 |
0.28 |
|
|
|
| 4 |
A2 |
223 |
223 |
0.00 |
|
|
|
| 5 |
B2 |
680 |
680 |
122.28 |
|
|
|
| 6 |
B2 |
346 |
346 |
0.22 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1248.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1248.6 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-pCVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.037 |
0.908 |
| S2 |
0.000 |
-1.037 |
0.908 |
| S3 |
0.000 |
1.593 |
-0.908 |
| S4 |
0.000 |
-1.593 |
-0.908 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0744 | 1.8983 | 3.1957 |
S2 | 2.0744 | | 3.1957 | 1.8983 | S3 | 1.8983 | 3.1957 | | 3.1859 | S4 | 3.1957 | 1.8983 | 3.1859 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.023 |
|
S1 |
S3 |
S4 |
72.977 |
| S2 |
S1 |
S3 |
107.023 |
|
S2 |
S4 |
S3 |
72.977 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.137 |
|
|
|
| 2 |
S |
0.137 |
|
|
|
| 3 |
S |
-0.137 |
|
|
|
| 4 |
S |
-0.137 |
|
|
|
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 |
1.430 |
1.430 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.914 |
0.000 |
0.000 |
| y |
0.000 |
-52.918 |
0.000 |
| z |
0.000 |
0.000 |
-48.296 |
|
| Traceless |
| | x | y | z |
| x |
-0.307 |
0.000 |
0.000 |
| y |
0.000 |
-3.313 |
0.000 |
| z |
0.000 |
0.000 |
3.620 |
|
| Polar |
| 3z2-r2 | 7.240 |
| x2-y2 | 2.004 |
| 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 |
5.935 |
0.000 |
0.000 |
| y |
0.000 |
18.131 |
0.000 |
| z |
0.000 |
0.000 |
11.731 |
<r2> (average value of r
2) Å
2
| <r2> |
200.011 |
| (<r2>)1/2 |
14.143 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.288265 |
| Energy at 298.15K | |
| HF Energy | -1592.288265 |
| Nuclear repulsion energy | 340.076061 |
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-pCVTZ
| 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 |
763 |
763 |
0.00 |
|
|
|
| 2 |
Ag |
312 |
312 |
0.00 |
|
|
|
| 3 |
Au |
263 |
263 |
0.00 |
|
|
|
| 4 |
B1u |
701 |
701 |
124.40 |
|
|
|
| 5 |
B2u |
170i |
170i |
18.17 |
|
|
|
| 6 |
B3g |
354 |
354 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1111.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1111.5 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 PBE1PBE/cc-pCVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.940 |
1.243 |
| S2 |
0.000 |
0.940 |
-1.243 |
| S3 |
0.000 |
-0.940 |
1.243 |
| S4 |
0.000 |
-0.940 |
-1.243 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4857 | 1.8798 | 3.1164 |
S2 | 2.4857 | | 3.1164 | 1.8798 | S3 | 1.8798 | 3.1164 | | 2.4857 | S4 | 3.1164 | 1.8798 | 2.4857 | |
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-pCVTZ
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 |
-51.254 |
0.000 |
0.000 |
| y |
0.000 |
-47.546 |
0.000 |
| z |
0.000 |
0.000 |
-52.592 |
|
| Traceless |
| | x | y | z |
| x |
-1.185 |
0.000 |
0.000 |
| y |
0.000 |
4.377 |
0.000 |
| z |
0.000 |
0.000 |
-3.192 |
|
| Polar |
| 3z2-r2 | -6.384 |
| x2-y2 | -3.708 |
| 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 |
5.912 |
0.000 |
0.000 |
| y |
0.000 |
12.243 |
0.000 |
| z |
0.000 |
0.000 |
17.038 |
<r2> (average value of r
2) Å
2
| <r2> |
186.910 |
| (<r2>)1/2 |
13.671 |