Jump to
S1C2
S1C3
Energy calculated at B3PW91/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.685776 |
| Energy at 298.15K | |
| HF Energy | -1592.685776 |
| Nuclear repulsion energy | 351.981667 |
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 B3PW91/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 |
531 |
531 |
0.00 |
|
|
|
| 2 |
A1 |
205 |
205 |
0.00 |
|
|
|
| 3 |
B1 |
470 |
470 |
0.00 |
|
|
|
| 4 |
B2 |
298 |
298 |
0.00 |
|
|
|
| 5 |
E |
440 |
440 |
0.00 |
|
|
|
| 5 |
E |
440 |
440 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1192.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1192.0 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 B3PW91/cc-pCVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.425 |
0.312 |
| S2 |
0.000 |
-1.425 |
0.312 |
| S3 |
-1.425 |
0.000 |
-0.312 |
| S4 |
1.425 |
0.000 |
-0.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8496 | 2.1093 | 2.1093 |
S2 | 2.8496 | | 2.1093 | 2.1093 | S3 | 2.1093 | 2.1093 | | 2.8496 | S4 | 2.1093 | 2.1093 | 2.8496 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.507 |
|
S1 |
S3 |
S4 |
47.507 |
| S2 |
S1 |
S3 |
47.507 |
|
S2 |
S4 |
S3 |
47.507 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/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 |
-48.468 |
0.000 |
0.000 |
| y |
0.000 |
-48.468 |
0.000 |
| z |
0.000 |
0.000 |
-53.905 |
|
| Traceless |
| | x | y | z |
| x |
2.718 |
0.000 |
0.000 |
| y |
0.000 |
2.718 |
0.000 |
| z |
0.000 |
0.000 |
-5.437 |
|
| Polar |
| 3z2-r2 | -10.873 |
| 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 |
11.352 |
0.000 |
0.000 |
| y |
0.000 |
11.352 |
0.000 |
| z |
0.000 |
0.000 |
6.755 |
<r2> (average value of r
2) Å
2
| <r2> |
167.551 |
| (<r2>)1/2 |
12.944 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.713136 |
| Energy at 298.15K | |
| HF Energy | -1592.713136 |
| Nuclear repulsion energy | 333.587115 |
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 B3PW91/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 |
699 |
699 |
6.83 |
|
|
|
| 2 |
A1 |
397 |
397 |
4.94 |
|
|
|
| 3 |
A1 |
111 |
111 |
0.31 |
|
|
|
| 4 |
A2 |
218 |
218 |
0.00 |
|
|
|
| 5 |
B2 |
670 |
670 |
117.20 |
|
|
|
| 6 |
B2 |
341 |
341 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1218.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1218.0 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 B3PW91/cc-pCVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.047 |
0.910 |
| S2 |
0.000 |
-1.047 |
0.910 |
| S3 |
0.000 |
1.603 |
-0.910 |
| S4 |
0.000 |
-1.603 |
-0.910 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0943 | 1.9032 | 3.2148 |
S2 | 2.0943 | | 3.2148 | 1.9032 | S3 | 1.9032 | 3.2148 | | 3.2053 | S4 | 3.2148 | 1.9032 | 3.2053 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.971 |
|
S1 |
S3 |
S4 |
73.029 |
| S2 |
S1 |
S3 |
106.971 |
|
S2 |
S4 |
S3 |
73.029 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.132 |
|
|
|
| 2 |
S |
0.132 |
|
|
|
| 3 |
S |
-0.132 |
|
|
|
| 4 |
S |
-0.132 |
|
|
|
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 |
1.392 |
1.392 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.833 |
0.000 |
0.000 |
| y |
0.000 |
-52.788 |
0.000 |
| z |
0.000 |
0.000 |
-48.232 |
|
| Traceless |
| | x | y | z |
| x |
-0.324 |
0.000 |
0.000 |
| y |
0.000 |
-3.255 |
0.000 |
| z |
0.000 |
0.000 |
3.579 |
|
| Polar |
| 3z2-r2 | 7.158 |
| x2-y2 | 1.954 |
| 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 |
5.942 |
0.000 |
0.000 |
| y |
0.000 |
18.267 |
0.000 |
| z |
0.000 |
0.000 |
11.833 |
<r2> (average value of r
2) Å
2
| <r2> |
201.914 |
| (<r2>)1/2 |
14.210 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.706891 |
| Energy at 298.15K | |
| HF Energy | -1592.706891 |
| Nuclear repulsion energy | 337.986429 |
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 B3PW91/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 |
748 |
748 |
0.00 |
|
|
|
| 2 |
Ag |
300 |
300 |
0.00 |
|
|
|
| 3 |
Au |
256 |
256 |
0.00 |
|
|
|
| 4 |
B1u |
689 |
689 |
119.20 |
|
|
|
| 5 |
B2u |
155i |
155i |
16.63 |
|
|
|
| 6 |
B3g |
347 |
347 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1092.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1092.9 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 B3PW91/cc-pCVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.943 |
1.255 |
| S2 |
0.000 |
0.943 |
-1.255 |
| S3 |
0.000 |
-0.943 |
1.255 |
| S4 |
0.000 |
-0.943 |
-1.255 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5091 | 1.8857 | 3.1387 |
S2 | 2.5091 | | 3.1387 | 1.8857 | S3 | 1.8857 | 3.1387 | | 2.5091 | S4 | 3.1387 | 1.8857 | 2.5091 | |
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 B3PW91/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 |
-51.165 |
0.000 |
0.000 |
| y |
0.000 |
-47.503 |
0.000 |
| z |
0.000 |
0.000 |
-52.443 |
|
| Traceless |
| | x | y | z |
| x |
-1.191 |
0.000 |
0.000 |
| y |
0.000 |
4.301 |
0.000 |
| z |
0.000 |
0.000 |
-3.110 |
|
| Polar |
| 3z2-r2 | -6.219 |
| x2-y2 | -3.662 |
| 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 |
5.923 |
0.000 |
0.000 |
| y |
0.000 |
12.347 |
0.000 |
| z |
0.000 |
0.000 |
17.196 |
<r2> (average value of r
2) Å
2
| <r2> |
189.082 |
| (<r2>)1/2 |
13.751 |