Jump to
S1C2
S1C3
Energy calculated at B97D3/3-21G
| | hartrees |
| Energy at 0K | -1584.878629 |
| Energy at 298.15K | |
| HF Energy | -1584.878629 |
| Nuclear repulsion energy | 312.753872 |
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 B97D3/3-21G
| 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 |
424 |
417 |
0.00 |
42.06 |
0.06 |
0.11 |
| 2 |
A1 |
150 |
148 |
0.00 |
10.21 |
0.75 |
0.86 |
| 3 |
B1 |
292 |
287 |
0.00 |
28.03 |
0.75 |
0.86 |
| 4 |
B2 |
248 |
244 |
0.10 |
20.69 |
0.75 |
0.86 |
| 5 |
E |
311 |
305 |
1.06 |
7.49 |
0.75 |
0.86 |
| 5 |
E |
311 |
305 |
1.06 |
7.49 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 867.5 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 852.7 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 B97D3/3-21G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.596 |
0.374 |
| S2 |
0.000 |
-1.596 |
0.374 |
| S3 |
-1.596 |
0.000 |
-0.374 |
| S4 |
1.596 |
0.000 |
-0.374 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.1922 | 2.3779 | 2.3779 |
S2 | 3.1922 | | 2.3779 | 2.3779 | S3 | 2.3779 | 2.3779 | | 3.1922 | S4 | 2.3779 | 2.3779 | 3.1922 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.839 |
|
S1 |
S3 |
S4 |
47.839 |
| S2 |
S1 |
S3 |
47.839 |
|
S2 |
S4 |
S3 |
47.839 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
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 |
-51.148 |
0.000 |
0.000 |
| y |
0.000 |
-51.148 |
0.000 |
| z |
0.000 |
0.000 |
-56.081 |
|
| Traceless |
| | x | y | z |
| x |
2.467 |
0.000 |
0.000 |
| y |
0.000 |
2.467 |
0.000 |
| z |
0.000 |
0.000 |
-4.934 |
|
| Polar |
| 3z2-r2 | -9.867 |
| 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 |
12.622 |
0.000 |
0.000 |
| y |
0.000 |
12.622 |
0.000 |
| z |
0.000 |
0.000 |
4.278 |
<r2> (average value of r
2) Å
2
| <r2> |
204.966 |
| (<r2>)1/2 |
14.317 |
Jump to
S1C1
S1C3
Energy calculated at B97D3/3-21G
| | hartrees |
| Energy at 0K | -1584.915867 |
| Energy at 298.15K | |
| HF Energy | -1584.915867 |
| Nuclear repulsion energy | 305.089113 |
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 B97D3/3-21G
| 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 |
535 |
526 |
0.00 |
31.22 |
0.27 |
0.43 |
| 2 |
A1 |
272 |
268 |
0.00 |
26.90 |
0.26 |
0.41 |
| 3 |
A1 |
141 |
139 |
5.83 |
0.00 |
0.68 |
0.81 |
| 4 |
A2 |
181 |
178 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
507 |
499 |
54.83 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
258 |
253 |
0.00 |
20.91 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 947.5 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 931.4 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 B97D3/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.385 |
1.048 |
| S2 |
0.000 |
-1.385 |
1.048 |
| S3 |
0.000 |
1.385 |
-1.048 |
| S4 |
0.000 |
-1.385 |
-1.048 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7708 | 2.0954 | 3.4737 |
S2 | 2.7708 | | 3.4737 | 2.0954 | S3 | 2.0954 | 3.4737 | | 2.7703 | S4 | 3.4737 | 2.0954 | 2.7703 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
89.993 |
|
S1 |
S3 |
S4 |
90.007 |
| S2 |
S1 |
S3 |
89.993 |
|
S2 |
S4 |
S3 |
90.007 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/3-21G
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 |
-0.001 |
0.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.915 |
0.000 |
0.000 |
| y |
0.000 |
-54.439 |
0.000 |
| z |
0.000 |
0.000 |
-51.273 |
|
| Traceless |
| | x | y | z |
| x |
-0.059 |
0.000 |
0.000 |
| y |
0.000 |
-2.345 |
0.000 |
| z |
0.000 |
0.000 |
2.404 |
|
| Polar |
| 3z2-r2 | 4.807 |
| x2-y2 | 1.524 |
| 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 |
2.835 |
0.000 |
0.000 |
| y |
0.000 |
16.796 |
0.000 |
| z |
0.000 |
0.000 |
13.286 |
<r2> (average value of r
2) Å
2
| <r2> |
226.094 |
| (<r2>)1/2 |
15.036 |
Jump to
S1C1
S1C2
Energy calculated at B97D3/3-21G
| | hartrees |
| Energy at 0K | -1584.915867 |
| Energy at 298.15K | |
| HF Energy | -1584.915867 |
| Nuclear repulsion energy | 305.109731 |
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 B97D3/3-21G
| 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 |
535 |
526 |
0.00 |
31.22 |
0.27 |
0.43 |
| 2 |
Ag |
272 |
268 |
0.00 |
26.90 |
0.26 |
0.41 |
| 3 |
Au |
181 |
178 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
508 |
499 |
54.85 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
141 |
139 |
5.83 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
258 |
253 |
0.00 |
20.91 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 947.7 cm
-1
Scaled (by 0.983) Zero Point Vibrational Energy (zpe) 931.6 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 B97D3/3-21G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.048 |
1.385 |
| S2 |
0.000 |
1.048 |
-1.385 |
| S3 |
0.000 |
-1.048 |
1.385 |
| S4 |
0.000 |
-1.048 |
-1.385 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7704 | 2.0953 | 3.4735 |
S2 | 2.7704 | | 3.4735 | 2.0953 | S3 | 2.0953 | 3.4735 | | 2.7704 | S4 | 3.4735 | 2.0953 | 2.7704 | |
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 B97D3/3-21G
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 |
-52.914 |
0.000 |
0.000 |
| y |
0.000 |
-51.274 |
0.000 |
| z |
0.000 |
0.000 |
-54.440 |
|
| Traceless |
| | x | y | z |
| x |
-0.057 |
0.000 |
0.000 |
| y |
0.000 |
2.403 |
0.000 |
| z |
0.000 |
0.000 |
-2.345 |
|
| Polar |
| 3z2-r2 | -4.690 |
| x2-y2 | -1.640 |
| 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 |
2.835 |
0.000 |
0.000 |
| y |
0.000 |
13.284 |
0.000 |
| z |
0.000 |
0.000 |
16.794 |
<r2> (average value of r
2) Å
2
| <r2> |
226.068 |
| (<r2>)1/2 |
15.036 |