Jump to
S1C2
S1C3
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -1584.675675 |
| Energy at 298.15K | |
| HF Energy | -1584.675675 |
| Nuclear repulsion energy | 348.740318 |
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 PBE1PBE/3-21G
| 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 |
496 |
477 |
0.00 |
47.80 |
0.07 |
0.13 |
| 2 |
A1 |
199 |
191 |
0.00 |
3.55 |
0.75 |
0.86 |
| 3 |
B1 |
424 |
408 |
0.00 |
32.46 |
0.75 |
0.86 |
| 4 |
B2 |
318 |
306 |
0.56 |
12.45 |
0.75 |
0.86 |
| 5 |
E |
401 |
385 |
0.08 |
7.10 |
0.75 |
0.86 |
| 5 |
E |
401 |
385 |
0.08 |
7.10 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1119.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 1075.3 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 PBE1PBE/3-21G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.438 |
0.315 |
| S2 |
0.000 |
-1.438 |
0.315 |
| S3 |
-1.438 |
0.000 |
-0.315 |
| S4 |
1.438 |
0.000 |
-0.315 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8757 | 2.1290 | 2.1290 |
S2 | 2.8757 | | 2.1290 | 2.1290 | S3 | 2.1290 | 2.1290 | | 2.8757 | S4 | 2.1290 | 2.1290 | 2.8757 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.518 |
|
S1 |
S3 |
S4 |
47.518 |
| S2 |
S1 |
S3 |
47.518 |
|
S2 |
S4 |
S3 |
47.518 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
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 |
-50.294 |
0.000 |
0.000 |
| y |
0.000 |
-50.294 |
0.000 |
| z |
0.000 |
0.000 |
-55.505 |
|
| Traceless |
| | x | y | z |
| x |
2.606 |
0.000 |
0.000 |
| y |
0.000 |
2.606 |
0.000 |
| z |
0.000 |
0.000 |
-5.211 |
|
| Polar |
| 3z2-r2 | -10.422 |
| 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 |
10.062 |
0.000 |
0.000 |
| y |
0.000 |
10.062 |
0.000 |
| z |
0.000 |
0.000 |
4.804 |
<r2> (average value of r
2) Å
2
| <r2> |
171.175 |
| (<r2>)1/2 |
13.083 |
Jump to
S1C1
S1C3
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -1584.711769 |
| Energy at 298.15K | |
| HF Energy | -1584.711769 |
| Nuclear repulsion energy | 333.479376 |
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 PBE1PBE/3-21G
| 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 |
717 |
688 |
1.99 |
29.62 |
0.25 |
0.40 |
| 2 |
A1 |
305 |
293 |
6.22 |
35.86 |
0.25 |
0.40 |
| 3 |
A1 |
97 |
94 |
4.14 |
4.01 |
0.63 |
0.78 |
| 4 |
A2 |
232 |
223 |
0.00 |
0.10 |
0.75 |
0.86 |
| 5 |
B2 |
685 |
657 |
129.85 |
1.65 |
0.75 |
0.86 |
| 6 |
B2 |
348 |
334 |
0.01 |
16.13 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1191.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 1144.5 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 PBE1PBE/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.094 |
0.926 |
| S2 |
0.000 |
-1.094 |
0.926 |
| S3 |
0.000 |
1.521 |
-0.926 |
| S4 |
0.000 |
-1.521 |
-0.926 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1881 | 1.9012 | 3.2050 |
S2 | 2.1881 | | 3.2050 | 1.9012 | S3 | 1.9012 | 3.2050 | | 3.0426 | S4 | 3.2050 | 1.9012 | 3.0426 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
102.987 |
|
S1 |
S3 |
S4 |
77.013 |
| S2 |
S1 |
S3 |
102.987 |
|
S2 |
S4 |
S3 |
77.013 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/3-21G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.074 |
|
|
|
| 2 |
S |
0.074 |
|
|
|
| 3 |
S |
-0.074 |
|
|
|
| 4 |
S |
-0.074 |
|
|
|
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 |
1.265 |
1.265 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.926 |
0.000 |
0.000 |
| y |
0.000 |
-54.301 |
0.000 |
| z |
0.000 |
0.000 |
-50.074 |
|
| Traceless |
| | x | y | z |
| x |
0.261 |
0.000 |
0.000 |
| y |
0.000 |
-3.301 |
0.000 |
| z |
0.000 |
0.000 |
3.040 |
|
| Polar |
| 3z2-r2 | 6.079 |
| x2-y2 | 2.375 |
| 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 |
3.883 |
0.000 |
0.000 |
| y |
0.000 |
16.376 |
0.000 |
| z |
0.000 |
0.000 |
10.841 |
<r2> (average value of r
2) Å
2
| <r2> |
199.817 |
| (<r2>)1/2 |
14.136 |
Jump to
S1C1
S1C2
Energy calculated at PBE1PBE/3-21G
| | hartrees |
| Energy at 0K | -1584.710936 |
| Energy at 298.15K | |
| HF Energy | -1584.710936 |
| Nuclear repulsion energy | 333.527332 |
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 PBE1PBE/3-21G
| 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 |
755 |
725 |
0.00 |
34.15 |
0.30 |
0.46 |
| 2 |
Ag |
297 |
286 |
0.00 |
33.32 |
0.28 |
0.44 |
| 3 |
Au |
251 |
241 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
702 |
674 |
143.30 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
53i |
51i |
15.03 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
345 |
331 |
0.00 |
17.62 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1148.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 1103.2 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 PBE1PBE/3-21G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.945 |
1.286 |
| S2 |
0.000 |
0.945 |
-1.286 |
| S3 |
0.000 |
-0.945 |
1.286 |
| S4 |
0.000 |
-0.945 |
-1.286 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5727 | 1.8901 | 3.1924 |
S2 | 2.5727 | | 3.1924 | 1.8901 | S3 | 1.8901 | 3.1924 | | 2.5727 | S4 | 3.1924 | 1.8901 | 2.5727 | |
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 PBE1PBE/3-21G
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 |
-52.211 |
0.000 |
0.000 |
| y |
0.000 |
-49.688 |
0.000 |
| z |
0.000 |
0.000 |
-53.886 |
|
| Traceless |
| | x | y | z |
| x |
-0.425 |
0.000 |
0.000 |
| y |
0.000 |
3.361 |
0.000 |
| z |
0.000 |
0.000 |
-2.936 |
|
| Polar |
| 3z2-r2 | -5.872 |
| x2-y2 | -2.524 |
| 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 |
3.841 |
0.000 |
0.000 |
| y |
0.000 |
11.269 |
0.000 |
| z |
0.000 |
0.000 |
16.049 |
<r2> (average value of r
2) Å
2
| <r2> |
195.494 |
| (<r2>)1/2 |
13.982 |