Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.305267 |
| Energy at 298.15K | |
| HF Energy | -1592.305267 |
| Nuclear repulsion energy | 353.512271 |
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/Def2TZVPP
| 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 |
540 |
540 |
0.00 |
36.57 |
0.05 |
0.09 |
| 2 |
A1 |
210 |
210 |
0.00 |
2.38 |
0.74 |
0.85 |
| 3 |
B1 |
479 |
479 |
0.00 |
16.11 |
0.75 |
0.86 |
| 4 |
B2 |
302 |
302 |
0.00 |
8.03 |
0.75 |
0.86 |
| 5 |
E |
450 |
450 |
0.00 |
4.09 |
0.75 |
0.86 |
| 5 |
E |
450 |
450 |
0.00 |
4.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1214.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1214.4 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/Def2TZVPP
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.418 |
0.314 |
| S2 |
0.000 |
-1.418 |
0.314 |
| S3 |
-1.418 |
0.000 |
-0.314 |
| S4 |
1.418 |
0.000 |
-0.314 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8352 | 2.1007 | 2.1007 |
S2 | 2.8352 | | 2.1007 | 2.1007 | S3 | 2.1007 | 2.1007 | | 2.8352 | S4 | 2.1007 | 2.1007 | 2.8352 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.561 |
|
S1 |
S3 |
S4 |
47.561 |
| S2 |
S1 |
S3 |
47.561 |
|
S2 |
S4 |
S3 |
47.561 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/Def2TZVPP
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 |
-48.594 |
0.000 |
0.000 |
| y |
0.000 |
-48.594 |
0.000 |
| z |
0.000 |
0.000 |
-54.001 |
|
| Traceless |
| | x | y | z |
| x |
2.703 |
0.000 |
0.000 |
| y |
0.000 |
2.703 |
0.000 |
| z |
0.000 |
0.000 |
-5.406 |
|
| Polar |
| 3z2-r2 | -10.813 |
| 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 |
11.211 |
0.000 |
0.000 |
| y |
0.000 |
11.211 |
0.000 |
| z |
0.000 |
0.000 |
6.577 |
<r2> (average value of r
2) Å
2
| <r2> |
166.390 |
| (<r2>)1/2 |
12.899 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.330801 |
| Energy at 298.15K | |
| HF Energy | -1592.330801 |
| Nuclear repulsion energy | 335.095465 |
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/Def2TZVPP
| 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 |
708 |
708 |
7.55 |
24.30 |
0.16 |
0.27 |
| 2 |
A1 |
412 |
412 |
4.90 |
40.04 |
0.19 |
0.32 |
| 3 |
A1 |
117 |
117 |
0.30 |
10.18 |
0.45 |
0.62 |
| 4 |
A2 |
223 |
223 |
0.00 |
0.11 |
0.75 |
0.86 |
| 5 |
B2 |
678 |
678 |
122.03 |
3.88 |
0.75 |
0.86 |
| 6 |
B2 |
346 |
346 |
0.19 |
11.12 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1241.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1241.6 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/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.039 |
0.907 |
| S2 |
0.000 |
-1.039 |
0.907 |
| S3 |
0.000 |
1.595 |
-0.907 |
| S4 |
0.000 |
-1.595 |
-0.907 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0783 | 1.8979 | 3.1989 |
S2 | 2.0783 | | 3.1989 | 1.8979 | S3 | 1.8979 | 3.1989 | | 3.1907 | S4 | 3.1989 | 1.8979 | 3.1907 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.041 |
|
S1 |
S3 |
S4 |
72.959 |
| S2 |
S1 |
S3 |
107.041 |
|
S2 |
S4 |
S3 |
72.959 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/Def2TZVPP
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 |
1.428 |
1.428 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.960 |
0.000 |
0.000 |
| y |
0.000 |
-53.007 |
0.000 |
| z |
0.000 |
0.000 |
-48.247 |
|
| Traceless |
| | x | y | z |
| x |
-0.333 |
0.000 |
0.000 |
| y |
0.000 |
-3.403 |
0.000 |
| z |
0.000 |
0.000 |
3.736 |
|
| Polar |
| 3z2-r2 | 7.472 |
| x2-y2 | 2.047 |
| 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 |
5.720 |
0.000 |
0.000 |
| y |
0.000 |
18.067 |
0.000 |
| z |
0.000 |
0.000 |
11.713 |
<r2> (average value of r
2) Å
2
| <r2> |
200.371 |
| (<r2>)1/2 |
14.155 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.323595 |
| Energy at 298.15K | |
| HF Energy | -1592.323595 |
| Nuclear repulsion energy | 339.410667 |
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/Def2TZVPP
| 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 |
760 |
760 |
0.00 |
32.17 |
0.20 |
0.34 |
| 2 |
Ag |
305 |
305 |
0.00 |
35.83 |
0.24 |
0.39 |
| 3 |
Au |
261 |
261 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
699 |
699 |
124.77 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
167i |
167i |
17.73 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
352 |
352 |
0.00 |
12.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1105.2 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1105.2 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/Def2TZVPP
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.940 |
1.248 |
| S2 |
0.000 |
0.940 |
-1.248 |
| S3 |
0.000 |
-0.940 |
1.248 |
| S4 |
0.000 |
-0.940 |
-1.248 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4958 | 1.8797 | 3.1245 |
S2 | 2.4958 | | 3.1245 | 1.8797 | S3 | 1.8797 | 3.1245 | | 2.4958 | S4 | 3.1245 | 1.8797 | 2.4958 | |
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/Def2TZVPP
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 |
-51.318 |
0.000 |
0.000 |
| y |
0.000 |
-47.508 |
0.000 |
| z |
0.000 |
0.000 |
-52.606 |
|
| Traceless |
| | x | y | z |
| x |
-1.260 |
0.000 |
0.000 |
| y |
0.000 |
4.454 |
0.000 |
| z |
0.000 |
0.000 |
-3.193 |
|
| Polar |
| 3z2-r2 | -6.387 |
| x2-y2 | -3.810 |
| 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 |
5.698 |
0.000 |
0.000 |
| y |
0.000 |
12.236 |
0.000 |
| z |
0.000 |
0.000 |
17.057 |
<r2> (average value of r
2) Å
2
| <r2> |
187.724 |
| (<r2>)1/2 |
13.701 |