Jump to
S1C2
S1C3
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -1585.296734 |
| Energy at 298.15K | |
| HF Energy | -1585.296734 |
| Nuclear repulsion energy | 341.496864 |
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 |
432 |
432 |
0.00 |
45.88 |
0.07 |
0.13 |
| 2 |
A1 |
187 |
187 |
0.00 |
4.23 |
0.75 |
0.86 |
| 3 |
B1 |
329 |
329 |
0.00 |
33.82 |
0.75 |
0.86 |
| 4 |
B2 |
295 |
295 |
0.29 |
15.38 |
0.75 |
0.86 |
| 5 |
E |
310 |
310 |
0.78 |
5.89 |
0.75 |
0.86 |
| 5 |
E |
310 |
310 |
0.78 |
5.89 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 930.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 930.8 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 B97D3/3-21G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.469 |
0.321 |
| S2 |
0.000 |
-1.469 |
0.321 |
| S3 |
-1.469 |
0.000 |
-0.321 |
| S4 |
1.469 |
0.000 |
-0.321 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9371 | 2.1740 | 2.1740 |
S2 | 2.9371 | | 2.1740 | 2.1740 | S3 | 2.1740 | 2.1740 | | 2.9371 | S4 | 2.1740 | 2.1740 | 2.9371 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.508 |
|
S1 |
S3 |
S4 |
47.508 |
| S2 |
S1 |
S3 |
47.508 |
|
S2 |
S4 |
S3 |
47.508 |
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 |
-49.721 |
0.000 |
0.000 |
| y |
0.000 |
-49.721 |
0.000 |
| z |
0.000 |
0.000 |
-55.000 |
|
| Traceless |
| | x | y | z |
| x |
2.640 |
0.000 |
0.000 |
| y |
0.000 |
2.640 |
0.000 |
| z |
0.000 |
0.000 |
-5.279 |
|
| Polar |
| 3z2-r2 | -10.558 |
| 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 |
10.546 |
0.000 |
0.000 |
| y |
0.000 |
10.546 |
0.000 |
| z |
0.000 |
0.000 |
4.863 |
<r2> (average value of r
2) Å
2
| <r2> |
176.789 |
| (<r2>)1/2 |
13.296 |
Jump to
S1C1
S1C3
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -1585.359419 |
| Energy at 298.15K | |
| HF Energy | -1585.359419 |
| Nuclear repulsion energy | 325.837758 |
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 |
702 |
702 |
0.00 |
32.10 |
0.29 |
0.44 |
| 2 |
A1 |
248 |
248 |
0.00 |
27.24 |
0.27 |
0.42 |
| 3 |
A1 |
49 |
49 |
8.80 |
0.00 |
0.48 |
0.65 |
| 4 |
A2 |
223 |
223 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
661 |
661 |
103.95 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
316 |
316 |
0.00 |
17.11 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1099.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1099.5 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 B97D3/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.334 |
0.956 |
| S2 |
0.000 |
-1.334 |
0.956 |
| S3 |
0.000 |
1.334 |
-0.956 |
| S4 |
0.000 |
-1.334 |
-0.956 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6674 | 1.9120 | 3.2818 |
S2 | 2.6674 | | 3.2818 | 1.9120 | S3 | 1.9120 | 3.2818 | | 2.6672 | S4 | 3.2818 | 1.9120 | 2.6672 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
89.998 |
|
S1 |
S3 |
S4 |
90.002 |
| S2 |
S1 |
S3 |
89.998 |
|
S2 |
S4 |
S3 |
90.002 |
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 |
-51.679 |
0.000 |
0.000 |
| y |
0.000 |
-52.911 |
0.000 |
| z |
0.000 |
0.000 |
-49.103 |
|
| Traceless |
| | x | y | z |
| x |
-0.672 |
0.000 |
0.000 |
| y |
0.000 |
-2.520 |
0.000 |
| z |
0.000 |
0.000 |
3.192 |
|
| Polar |
| 3z2-r2 | 6.383 |
| x2-y2 | 1.232 |
| 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 |
3.859 |
0.000 |
0.000 |
| y |
0.000 |
16.203 |
0.000 |
| z |
0.000 |
0.000 |
11.513 |
<r2> (average value of r
2) Å
2
| <r2> |
204.322 |
| (<r2>)1/2 |
14.294 |
Jump to
S1C1
S1C2
Energy calculated at B97D3/3-21G*
| | hartrees |
| Energy at 0K | -1585.359419 |
| Energy at 298.15K | |
| HF Energy | -1585.359419 |
| Nuclear repulsion energy | 325.857072 |
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 |
702 |
702 |
0.00 |
32.10 |
0.29 |
0.44 |
| 2 |
Ag |
248 |
248 |
0.00 |
27.24 |
0.27 |
0.42 |
| 3 |
Au |
223 |
223 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
661 |
661 |
103.96 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
49 |
49 |
8.81 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
316 |
316 |
0.00 |
17.11 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1099.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1099.7 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 D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.956 |
1.334 |
| S2 |
0.000 |
0.956 |
-1.334 |
| S3 |
0.000 |
-0.956 |
1.334 |
| S4 |
0.000 |
-0.956 |
-1.334 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6671 | 1.9120 | 3.2816 |
S2 | 2.6671 | | 3.2816 | 1.9120 | S3 | 1.9120 | 3.2816 | | 2.6671 | S4 | 3.2816 | 1.9120 | 2.6671 | |
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 |
-51.678 |
0.000 |
0.000 |
| y |
0.000 |
-49.103 |
0.000 |
| z |
0.000 |
0.000 |
-52.911 |
|
| Traceless |
| | x | y | z |
| x |
-0.671 |
0.000 |
0.000 |
| y |
0.000 |
3.192 |
0.000 |
| z |
0.000 |
0.000 |
-2.520 |
|
| Polar |
| 3z2-r2 | -5.041 |
| x2-y2 | -2.575 |
| 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 |
3.859 |
0.000 |
0.000 |
| y |
0.000 |
11.512 |
0.000 |
| z |
0.000 |
0.000 |
16.201 |
<r2> (average value of r
2) Å
2
| <r2> |
204.299 |
| (<r2>)1/2 |
14.293 |