Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-31G**
| | hartrees |
| Energy at 0K | -1592.154037 |
| Energy at 298.15K | |
| HF Energy | -1592.154037 |
| Nuclear repulsion energy | 348.640244 |
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 HSEh1PBE/6-31G**
| 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 |
514 |
490 |
0.00 |
51.83 |
0.07 |
0.13 |
| 2 |
A1 |
199 |
190 |
0.00 |
2.83 |
0.75 |
0.86 |
| 3 |
B1 |
448 |
428 |
0.00 |
36.13 |
0.75 |
0.86 |
| 4 |
B2 |
312 |
298 |
0.42 |
11.44 |
0.75 |
0.86 |
| 5 |
E |
429 |
409 |
0.08 |
7.07 |
0.75 |
0.86 |
| 5 |
E |
429 |
409 |
0.08 |
7.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1164.9 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 1111.6 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 HSEh1PBE/6-31G**
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.439 |
0.313 |
| S2 |
0.000 |
-1.439 |
0.313 |
| S3 |
-1.439 |
0.000 |
-0.313 |
| S4 |
1.439 |
0.000 |
-0.313 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8783 | 2.1291 | 2.1291 |
S2 | 2.8783 | | 2.1291 | 2.1291 | S3 | 2.1291 | 2.1291 | | 2.8783 | S4 | 2.1291 | 2.1291 | 2.8783 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.473 |
|
S1 |
S3 |
S4 |
47.473 |
| S2 |
S1 |
S3 |
47.473 |
|
S2 |
S4 |
S3 |
47.473 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
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 |
-49.829 |
0.000 |
0.000 |
| y |
0.000 |
-49.829 |
0.000 |
| z |
0.000 |
0.000 |
-55.083 |
|
| Traceless |
| | x | y | z |
| x |
2.627 |
0.000 |
0.000 |
| y |
0.000 |
2.627 |
0.000 |
| z |
0.000 |
0.000 |
-5.254 |
|
| Polar |
| 3z2-r2 | -10.508 |
| 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 |
10.372 |
0.000 |
0.000 |
| y |
0.000 |
10.372 |
0.000 |
| z |
0.000 |
0.000 |
5.328 |
<r2> (average value of r
2) Å
2
| <r2> |
171.023 |
| (<r2>)1/2 |
13.078 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-31G**
| | hartrees |
| Energy at 0K | -1592.185136 |
| Energy at 298.15K | |
| HF Energy | -1592.185136 |
| Nuclear repulsion energy | 330.133289 |
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 HSEh1PBE/6-31G**
| 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 |
691 |
659 |
2.64 |
30.80 |
0.23 |
0.38 |
| 2 |
A1 |
355 |
339 |
7.29 |
34.36 |
0.23 |
0.37 |
| 3 |
A1 |
106 |
101 |
0.97 |
9.80 |
0.50 |
0.67 |
| 4 |
A2 |
216 |
207 |
0.00 |
0.20 |
0.75 |
0.86 |
| 5 |
B2 |
667 |
636 |
130.92 |
2.69 |
0.75 |
0.86 |
| 6 |
B2 |
336 |
321 |
0.04 |
15.43 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1185.0 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 1130.8 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 HSEh1PBE/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.073 |
0.923 |
| S2 |
0.000 |
-1.073 |
0.923 |
| S3 |
0.000 |
1.599 |
-0.923 |
| S4 |
0.000 |
-1.599 |
-0.923 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1464 | 1.9186 | 3.2472 |
S2 | 2.1464 | | 3.2472 | 1.9186 | S3 | 1.9186 | 3.2472 | | 3.1976 | S4 | 3.2472 | 1.9186 | 3.1976 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
105.899 |
|
S1 |
S3 |
S4 |
74.101 |
| S2 |
S1 |
S3 |
105.899 |
|
S2 |
S4 |
S3 |
74.101 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.099 |
|
|
|
| 2 |
S |
0.099 |
|
|
|
| 3 |
S |
-0.099 |
|
|
|
| 4 |
S |
-0.099 |
|
|
|
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 |
1.519 |
1.519 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.559 |
0.000 |
0.000 |
| y |
0.000 |
-54.239 |
0.000 |
| z |
0.000 |
0.000 |
-49.906 |
|
| Traceless |
| | x | y | z |
| x |
0.514 |
0.000 |
0.000 |
| y |
0.000 |
-3.506 |
0.000 |
| z |
0.000 |
0.000 |
2.992 |
|
| Polar |
| 3z2-r2 | 5.985 |
| x2-y2 | 2.680 |
| 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 |
4.342 |
0.000 |
0.000 |
| y |
0.000 |
17.696 |
0.000 |
| z |
0.000 |
0.000 |
11.161 |
<r2> (average value of r
2) Å
2
| <r2> |
205.547 |
| (<r2>)1/2 |
14.337 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-31G**
| | hartrees |
| Energy at 0K | -1592.181827 |
| Energy at 298.15K | |
| HF Energy | -1592.181827 |
| Nuclear repulsion energy | 332.848848 |
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 HSEh1PBE/6-31G**
| 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 |
740 |
706 |
0.00 |
38.35 |
0.28 |
0.44 |
| 2 |
Ag |
287 |
274 |
0.00 |
33.43 |
0.29 |
0.44 |
| 3 |
Au |
248 |
236 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
690 |
659 |
144.03 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
106i |
101i |
18.61 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
337 |
322 |
0.00 |
17.44 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1098.0 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 1047.9 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 HSEh1PBE/6-31G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.951 |
1.283 |
| S2 |
0.000 |
0.951 |
-1.283 |
| S3 |
0.000 |
-0.951 |
1.283 |
| S4 |
0.000 |
-0.951 |
-1.283 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5656 | 1.9024 | 3.1940 |
S2 | 2.5656 | | 3.1940 | 1.9024 | S3 | 1.9024 | 3.1940 | | 2.5656 | S4 | 3.1940 | 1.9024 | 2.5656 | |
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 HSEh1PBE/6-31G**
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 |
-51.929 |
0.000 |
0.000 |
| y |
0.000 |
-49.272 |
0.000 |
| z |
0.000 |
0.000 |
-53.889 |
|
| Traceless |
| | x | y | z |
| x |
-0.349 |
0.000 |
0.000 |
| y |
0.000 |
3.637 |
0.000 |
| z |
0.000 |
0.000 |
-3.288 |
|
| Polar |
| 3z2-r2 | -6.576 |
| x2-y2 | -2.657 |
| 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 |
4.300 |
0.000 |
0.000 |
| y |
0.000 |
11.722 |
0.000 |
| z |
0.000 |
0.000 |
16.819 |
<r2> (average value of r
2) Å
2
| <r2> |
195.515 |
| (<r2>)1/2 |
13.983 |