Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.202396 |
| Energy at 298.15K | |
| HF Energy | -1592.202396 |
| Nuclear repulsion energy | 352.536724 |
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(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 |
543 |
520 |
0.00 |
38.49 |
0.04 |
0.08 |
| 2 |
A1 |
207 |
198 |
0.00 |
1.69 |
0.75 |
0.86 |
| 3 |
B1 |
483 |
463 |
0.00 |
18.52 |
0.75 |
0.86 |
| 4 |
B2 |
301 |
288 |
0.01 |
8.95 |
0.75 |
0.86 |
| 5 |
E |
455 |
436 |
0.01 |
4.18 |
0.75 |
0.86 |
| 5 |
E |
455 |
436 |
0.01 |
4.18 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1222.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1170.4 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 HSEh1PBE/6-31G(2df,p)
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.422 |
0.312 |
| S2 |
0.000 |
-1.422 |
0.312 |
| S3 |
-1.422 |
0.000 |
-0.312 |
| S4 |
1.422 |
0.000 |
-0.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8444 | 2.1062 | 2.1062 |
S2 | 2.8444 | | 2.1062 | 2.1062 | S3 | 2.1062 | 2.1062 | | 2.8444 | S4 | 2.1062 | 2.1062 | 2.8444 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.526 |
|
S1 |
S3 |
S4 |
47.526 |
| S2 |
S1 |
S3 |
47.526 |
|
S2 |
S4 |
S3 |
47.526 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
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 |
-48.576 |
0.000 |
0.000 |
| y |
0.000 |
-48.576 |
0.000 |
| z |
0.000 |
0.000 |
-53.998 |
|
| Traceless |
| | x | y | z |
| x |
2.711 |
0.000 |
0.000 |
| y |
0.000 |
2.711 |
0.000 |
| z |
0.000 |
0.000 |
-5.422 |
|
| Polar |
| 3z2-r2 | -10.845 |
| 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 |
11.015 |
0.000 |
0.000 |
| y |
0.000 |
11.015 |
0.000 |
| z |
0.000 |
0.000 |
6.740 |
<r2> (average value of r
2) Å
2
| <r2> |
167.167 |
| (<r2>)1/2 |
12.929 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.226071 |
| Energy at 298.15K | |
| HF Energy | -1592.226071 |
| Nuclear repulsion energy | 333.830067 |
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(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 |
707 |
677 |
6.62 |
26.32 |
0.16 |
0.27 |
| 2 |
A1 |
415 |
397 |
5.55 |
37.85 |
0.18 |
0.31 |
| 3 |
A1 |
117 |
112 |
0.33 |
11.00 |
0.46 |
0.63 |
| 4 |
A2 |
220 |
210 |
0.00 |
0.22 |
0.75 |
0.86 |
| 5 |
B2 |
680 |
651 |
119.67 |
3.15 |
0.75 |
0.86 |
| 6 |
B2 |
343 |
328 |
0.26 |
11.78 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1240.4 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1187.9 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(2df,p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.044 |
0.912 |
| S2 |
0.000 |
-1.044 |
0.912 |
| S3 |
0.000 |
1.598 |
-0.912 |
| S4 |
0.000 |
-1.598 |
-0.912 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0879 | 1.9058 | 3.2103 |
S2 | 2.0879 | | 3.2103 | 1.9058 | S3 | 1.9058 | 3.2103 | | 3.1965 | S4 | 3.2103 | 1.9058 | 3.1965 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.910 |
|
S1 |
S3 |
S4 |
73.090 |
| S2 |
S1 |
S3 |
106.910 |
|
S2 |
S4 |
S3 |
73.090 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.138 |
|
|
|
| 2 |
S |
0.138 |
|
|
|
| 3 |
S |
-0.138 |
|
|
|
| 4 |
S |
-0.138 |
|
|
|
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 |
1.452 |
1.452 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.911 |
0.000 |
0.000 |
| y |
0.000 |
-52.810 |
0.000 |
| z |
0.000 |
0.000 |
-48.310 |
|
| Traceless |
| | x | y | z |
| x |
-0.352 |
0.000 |
0.000 |
| y |
0.000 |
-3.199 |
0.000 |
| z |
0.000 |
0.000 |
3.551 |
|
| Polar |
| 3z2-r2 | 7.102 |
| x2-y2 | 1.898 |
| 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 |
5.872 |
0.000 |
0.000 |
| y |
0.000 |
17.829 |
0.000 |
| z |
0.000 |
0.000 |
11.477 |
<r2> (average value of r
2) Å
2
| <r2> |
201.462 |
| (<r2>)1/2 |
14.194 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -1592.218923 |
| Energy at 298.15K | |
| HF Energy | -1592.218923 |
| Nuclear repulsion energy | 338.325820 |
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(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 |
759 |
727 |
0.00 |
33.85 |
0.20 |
0.34 |
| 2 |
Ag |
305 |
292 |
0.00 |
35.04 |
0.25 |
0.40 |
| 3 |
Au |
259 |
248 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
701 |
671 |
126.17 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
167i |
160i |
18.16 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
350 |
335 |
0.00 |
13.94 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1102.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1056.1 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 HSEh1PBE/6-31G(2df,p)
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.944 |
1.251 |
| S2 |
0.000 |
0.944 |
-1.251 |
| S3 |
0.000 |
-0.944 |
1.251 |
| S4 |
0.000 |
-0.944 |
-1.251 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5016 | 1.8873 | 3.1337 |
S2 | 2.5016 | | 3.1337 | 1.8873 | S3 | 1.8873 | 3.1337 | | 2.5016 | S4 | 3.1337 | 1.8873 | 2.5016 | |
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(2df,p)
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 |
-51.231 |
0.000 |
0.000 |
| y |
0.000 |
-47.566 |
0.000 |
| z |
0.000 |
0.000 |
-52.540 |
|
| Traceless |
| | x | y | z |
| x |
-1.178 |
0.000 |
0.000 |
| y |
0.000 |
4.320 |
0.000 |
| z |
0.000 |
0.000 |
-3.142 |
|
| Polar |
| 3z2-r2 | -6.283 |
| x2-y2 | -3.666 |
| 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 |
5.905 |
0.000 |
0.000 |
| y |
0.000 |
11.997 |
0.000 |
| z |
0.000 |
0.000 |
16.736 |
<r2> (average value of r
2) Å
2
| <r2> |
188.625 |
| (<r2>)1/2 |
13.734 |