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S1C2
S1C3
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.197210 |
| Energy at 298.15K | |
| HF Energy | -1591.953555 |
| Nuclear repulsion energy | 349.846082 |
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=FULL/6-31G(2df,p)
| 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 |
524 |
524 |
0.00 |
39.43 |
0.04 |
0.09 |
| 2 |
A1 |
203 |
203 |
0.00 |
1.81 |
0.75 |
0.86 |
| 3 |
B1 |
464 |
464 |
0.00 |
19.03 |
0.75 |
0.86 |
| 4 |
B2 |
302 |
302 |
0.00 |
9.13 |
0.75 |
0.86 |
| 5 |
E |
436 |
436 |
0.02 |
4.40 |
0.75 |
0.86 |
| 5 |
E |
436 |
436 |
0.02 |
4.40 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1182.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1182.7 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=FULL/6-31G(2df,p)
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.433 |
0.314 |
| S2 |
0.000 |
-1.433 |
0.314 |
| S3 |
-1.433 |
0.000 |
-0.314 |
| S4 |
1.433 |
0.000 |
-0.314 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8670 | 2.1222 | 2.1222 |
S2 | 2.8670 | | 2.1222 | 2.1222 | S3 | 2.1222 | 2.1222 | | 2.8670 | S4 | 2.1222 | 2.1222 | 2.8670 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.508 |
|
S1 |
S3 |
S4 |
47.508 |
| S2 |
S1 |
S3 |
47.508 |
|
S2 |
S4 |
S3 |
47.508 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.233329 |
| Energy at 298.15K | |
| HF Energy | -1591.941050 |
| Nuclear repulsion energy | 330.743333 |
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=FULL/6-31G(2df,p)
| 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 |
701 |
701 |
0.00 |
35.27 |
0.16 |
0.27 |
| 2 |
A1 |
250 |
250 |
0.00 |
2.06 |
0.75 |
0.86 |
| 3 |
A1 |
94 |
94 |
8.56 |
0.00 |
0.63 |
0.77 |
| 4 |
A2 |
234 |
234 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
682 |
682 |
42.85 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
320 |
320 |
0.00 |
13.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1139.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1139.9 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 B2PLYP=FULL/6-31G(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.294 |
0.956 |
| S2 |
0.000 |
-1.294 |
0.956 |
| S3 |
0.000 |
1.293 |
-0.956 |
| S4 |
0.000 |
-1.293 |
-0.956 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5871 | 1.9112 | 3.2163 |
S2 | 2.5871 | | 3.2163 | 1.9112 | S3 | 1.9112 | 3.2163 | | 2.5866 | S4 | 3.2163 | 1.9112 | 2.5866 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
89.993 |
|
S1 |
S3 |
S4 |
90.007 |
| S2 |
S1 |
S3 |
89.993 |
|
S2 |
S4 |
S3 |
90.007 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP=FULL/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.233329 |
| Energy at 298.15K | |
| HF Energy | -1591.941059 |
| Nuclear repulsion energy | 330.764915 |
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=FULL/6-31G(2df,p)
| 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 |
700 |
700 |
0.00 |
35.27 |
0.16 |
0.27 |
| 2 |
Ag |
250 |
250 |
0.00 |
2.03 |
0.75 |
0.86 |
| 3 |
Au |
234 |
234 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
681 |
681 |
42.89 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
94 |
94 |
8.57 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
320 |
320 |
0.00 |
13.26 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1140.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1140.1 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 B2PLYP=FULL/6-31G(2df,p)
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.956 |
1.293 |
| S2 |
0.000 |
0.956 |
-1.293 |
| S3 |
0.000 |
-0.956 |
1.293 |
| S4 |
0.000 |
-0.956 |
-1.293 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5865 | 1.9112 | 3.2160 |
S2 | 2.5865 | | 3.2160 | 1.9112 | S3 | 1.9112 | 3.2160 | | 2.5865 | S4 | 3.2160 | 1.9112 | 2.5865 | |
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