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S1C2
S1C3
Energy calculated at B2PLYP=FULLultrafine/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.215170 |
| Energy at 298.15K | |
| HF Energy | -1592.015736 |
| Nuclear repulsion energy | 343.786204 |
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/daug-cc-pVDZ
| 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 |
500 |
500 |
0.00 |
47.16 |
0.04 |
0.08 |
| 2 |
A1 |
198 |
198 |
0.00 |
1.19 |
0.72 |
0.84 |
| 3 |
B1 |
431 |
431 |
0.00 |
19.10 |
0.75 |
0.86 |
| 4 |
B2 |
301 |
301 |
0.04 |
7.60 |
0.75 |
0.86 |
| 5 |
E |
409 |
409 |
0.04 |
3.66 |
0.75 |
0.86 |
| 5 |
E |
409 |
409 |
0.04 |
3.66 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1123.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1123.8 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/daug-cc-pVDZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.457 |
0.325 |
| S2 |
0.000 |
-1.457 |
0.325 |
| S3 |
-1.457 |
0.000 |
-0.325 |
| S4 |
1.457 |
0.000 |
-0.325 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9142 | 2.1605 | 2.1605 |
S2 | 2.9142 | | 2.1605 | 2.1605 | S3 | 2.1605 | 2.1605 | | 2.9142 | S4 | 2.1605 | 2.1605 | 2.9142 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.590 |
|
S1 |
S3 |
S4 |
47.590 |
| S2 |
S1 |
S3 |
47.590 |
|
S2 |
S4 |
S3 |
47.590 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Energy calculated at B2PLYP=FULLultrafine/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.257521 |
| Energy at 298.15K | |
| HF Energy | -1592.005125 |
| Nuclear repulsion energy | 324.343272 |
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/daug-cc-pVDZ
| 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 |
669 |
669 |
0.00 |
43.10 |
0.08 |
0.15 |
| 2 |
A1 |
236 |
236 |
0.00 |
18.61 |
0.59 |
0.74 |
| 3 |
A1 |
128 |
128 |
6.34 |
0.00 |
0.73 |
0.85 |
| 4 |
A2 |
216 |
216 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
655 |
655 |
34.16 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
301 |
301 |
0.00 |
8.17 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1102.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1102.0 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 B2PLYP=FULLultrafine/daug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.324 |
0.971 |
| S2 |
0.000 |
-1.324 |
0.971 |
| S3 |
0.000 |
1.324 |
-0.971 |
| S4 |
0.000 |
-1.324 |
-0.971 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6480 | 1.9417 | 3.2840 |
S2 | 2.6480 | | 3.2840 | 1.9417 | S3 | 1.9417 | 3.2840 | | 2.6489 | S4 | 3.2840 | 1.9417 | 2.6489 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.013 |
|
S1 |
S3 |
S4 |
89.987 |
| S2 |
S1 |
S3 |
90.013 |
|
S2 |
S4 |
S3 |
89.987 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP=FULLultrafine/daug-cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.257521 |
| Energy at 298.15K | |
| HF Energy | -1592.005155 |
| Nuclear repulsion energy | 324.392927 |
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/daug-cc-pVDZ
| 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 |
669 |
669 |
0.00 |
43.10 |
0.08 |
0.15 |
| 2 |
Ag |
236 |
236 |
0.00 |
18.17 |
0.59 |
0.74 |
| 3 |
Au |
216 |
216 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
655 |
655 |
34.29 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
128 |
128 |
6.36 |
0.00 |
0.34 |
0.50 |
| 6 |
B3g |
301 |
301 |
0.00 |
8.17 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1102.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1102.4 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 B2PLYP=FULLultrafine/daug-cc-pVDZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.971 |
1.324 |
| S2 |
0.000 |
0.971 |
-1.324 |
| S3 |
0.000 |
-0.971 |
1.324 |
| S4 |
0.000 |
-0.971 |
-1.324 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6477 | 1.9416 | 3.2833 |
S2 | 2.6477 | | 3.2833 | 1.9416 | S3 | 1.9416 | 3.2833 | | 2.6477 | S4 | 3.2833 | 1.9416 | 2.6477 | |
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