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S1C2
S1C3
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -1592.310183 |
| Energy at 298.15K | |
| HF Energy | -1592.002317 |
| Nuclear repulsion energy | 345.019594 |
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 B2PLYP=FULLultrafine/6-311G*
| 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 |
489 |
489 |
0.00 |
55.24 |
0.08 |
0.14 |
| 2 |
A1 |
196 |
196 |
0.00 |
3.77 |
0.69 |
0.82 |
| 3 |
B1 |
423 |
423 |
0.00 |
37.42 |
0.75 |
0.86 |
| 4 |
B2 |
304 |
304 |
0.04 |
9.56 |
0.75 |
0.86 |
| 5 |
E |
403 |
403 |
0.09 |
8.13 |
0.75 |
0.86 |
| 5 |
E |
403 |
403 |
0.09 |
8.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1108.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1108.8 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 B2PLYP=FULLultrafine/6-311G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.452 |
0.322 |
| S2 |
0.000 |
-1.452 |
0.322 |
| S3 |
-1.452 |
0.000 |
-0.322 |
| S4 |
1.452 |
0.000 |
-0.322 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9048 | 2.1525 | 2.1525 |
S2 | 2.9048 | | 2.1525 | 2.1525 | S3 | 2.1525 | 2.1525 | | 2.9048 | S4 | 2.1525 | 2.1525 | 2.9048 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.564 |
|
S1 |
S3 |
S4 |
47.564 |
| S2 |
S1 |
S3 |
47.564 |
|
S2 |
S4 |
S3 |
47.564 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -1592.353389 |
| Energy at 298.15K | |
| HF Energy | -1591.992295 |
| Nuclear repulsion energy | 323.733222 |
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 B2PLYP=FULLultrafine/6-311G*
| 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 |
659 |
659 |
0.00 |
43.45 |
0.22 |
0.37 |
| 2 |
A1 |
218 |
218 |
0.00 |
34.24 |
0.44 |
0.61 |
| 3 |
A1 |
117 |
117 |
10.23 |
0.00 |
0.35 |
0.52 |
| 4 |
A2 |
215 |
215 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
647 |
647 |
49.18 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
297 |
297 |
0.00 |
15.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1076.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1076.8 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 B2PLYP=FULLultrafine/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.340 |
0.964 |
| S2 |
0.000 |
-1.340 |
0.964 |
| S3 |
0.000 |
1.340 |
-0.964 |
| S4 |
0.000 |
-1.340 |
-0.964 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6799 | 1.9275 | 3.3012 |
S2 | 2.6799 | | 3.3012 | 1.9275 | S3 | 1.9275 | 3.3012 | | 2.6803 | S4 | 3.3012 | 1.9275 | 2.6803 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.005 |
|
S1 |
S3 |
S4 |
89.995 |
| S2 |
S1 |
S3 |
90.005 |
|
S2 |
S4 |
S3 |
89.995 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP=FULLultrafine/6-311G*
| | hartrees |
| Energy at 0K | -1592.353389 |
| Energy at 298.15K | |
| HF Energy | -1591.992290 |
| Nuclear repulsion energy | 323.728678 |
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 B2PLYP=FULLultrafine/6-311G*
| 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 |
659 |
659 |
0.00 |
43.45 |
0.22 |
0.37 |
| 2 |
Ag |
218 |
218 |
0.00 |
34.19 |
0.44 |
0.61 |
| 3 |
Au |
215 |
215 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
647 |
647 |
49.17 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
117 |
117 |
10.23 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
297 |
297 |
0.00 |
15.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1076.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1076.8 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 B2PLYP=FULLultrafine/6-311G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.964 |
1.340 |
| S2 |
0.000 |
0.964 |
-1.340 |
| S3 |
0.000 |
-0.964 |
1.340 |
| S4 |
0.000 |
-0.964 |
-1.340 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6800 | 1.9276 | 3.3012 |
S2 | 2.6800 | | 3.3012 | 1.9276 | S3 | 1.9276 | 3.3012 | | 2.6800 | S4 | 3.3012 | 1.9276 | 2.6800 | |
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