Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -1592.673924 |
| Energy at 298.15K | |
| HF Energy | -1592.673924 |
| Nuclear repulsion energy | 348.157825 |
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 M06-2X/6-311G*
| 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 |
521 |
521 |
0.00 |
60.33 |
0.08 |
0.15 |
| 2 |
A1 |
196 |
196 |
0.00 |
3.45 |
0.67 |
0.80 |
| 3 |
B1 |
465 |
465 |
0.00 |
39.76 |
0.75 |
0.86 |
| 4 |
B2 |
318 |
318 |
0.08 |
9.07 |
0.75 |
0.86 |
| 5 |
E |
445 |
445 |
0.00 |
8.83 |
0.75 |
0.86 |
| 5 |
E |
445 |
445 |
0.00 |
8.83 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1194.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1194.8 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 M06-2X/6-311G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.439 |
0.318 |
| S2 |
0.000 |
-1.439 |
0.318 |
| S3 |
-1.439 |
0.000 |
-0.318 |
| S4 |
1.439 |
0.000 |
-0.318 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8789 | 2.1330 | 2.1330 |
S2 | 2.8789 | | 2.1330 | 2.1330 | S3 | 2.1330 | 2.1330 | | 2.8789 | S4 | 2.1330 | 2.1330 | 2.8789 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.558 |
|
S1 |
S3 |
S4 |
47.558 |
| S2 |
S1 |
S3 |
47.558 |
|
S2 |
S4 |
S3 |
47.558 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
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 |
-50.670 |
0.000 |
0.000 |
| y |
0.000 |
-50.670 |
0.000 |
| z |
0.000 |
0.000 |
-55.914 |
|
| Traceless |
| | x | y | z |
| x |
2.622 |
0.000 |
0.000 |
| y |
0.000 |
2.622 |
0.000 |
| z |
0.000 |
0.000 |
-5.244 |
|
| Polar |
| 3z2-r2 | -10.488 |
| 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 |
10.825 |
0.000 |
0.000 |
| y |
0.000 |
10.825 |
0.000 |
| z |
0.000 |
0.000 |
5.599 |
<r2> (average value of r
2) Å
2
| <r2> |
171.837 |
| (<r2>)1/2 |
13.109 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -1592.682666 |
| Energy at 298.15K | |
| HF Energy | -1592.682666 |
| Nuclear repulsion energy | 332.279439 |
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 M06-2X/6-311G*
| 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 |
675 |
675 |
3.64 |
37.12 |
0.19 |
0.32 |
| 2 |
A1 |
392 |
392 |
8.63 |
59.49 |
0.25 |
0.40 |
| 3 |
A1 |
127 |
127 |
0.89 |
15.33 |
0.45 |
0.62 |
| 4 |
A2 |
217 |
217 |
0.00 |
0.42 |
0.75 |
0.86 |
| 5 |
B2 |
645 |
645 |
218.44 |
5.48 |
0.75 |
0.86 |
| 6 |
B2 |
338 |
338 |
0.16 |
12.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1196.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1196.9 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 M06-2X/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.052 |
0.918 |
| S2 |
0.000 |
-1.052 |
0.918 |
| S3 |
0.000 |
1.597 |
-0.918 |
| S4 |
0.000 |
-1.597 |
-0.918 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1039 | 1.9156 | 3.2235 |
S2 | 2.1039 | | 3.2235 | 1.9156 | S3 | 1.9156 | 3.2235 | | 3.1947 | S4 | 3.2235 | 1.9156 | 3.1947 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.542 |
|
S1 |
S3 |
S4 |
73.458 |
| S2 |
S1 |
S3 |
106.542 |
|
S2 |
S4 |
S3 |
73.458 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.141 |
|
|
|
| 2 |
S |
0.141 |
|
|
|
| 3 |
S |
-0.141 |
|
|
|
| 4 |
S |
-0.141 |
|
|
|
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 |
1.998 |
1.998 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.635 |
0.000 |
0.000 |
| y |
0.000 |
-56.092 |
0.000 |
| z |
0.000 |
0.000 |
-50.946 |
|
| Traceless |
| | x | y | z |
| x |
0.884 |
0.000 |
0.000 |
| y |
0.000 |
-4.301 |
0.000 |
| z |
0.000 |
0.000 |
3.417 |
|
| Polar |
| 3z2-r2 | 6.834 |
| x2-y2 | 3.457 |
| 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 |
4.567 |
0.000 |
0.000 |
| y |
0.000 |
20.398 |
0.000 |
| z |
0.000 |
0.000 |
11.601 |
<r2> (average value of r
2) Å
2
| <r2> |
204.260 |
| (<r2>)1/2 |
14.292 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -1592.676969 |
| Energy at 298.15K | |
| HF Energy | -1592.676969 |
| Nuclear repulsion energy | 336.381984 |
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 M06-2X/6-311G*
| 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 |
750 |
750 |
0.00 |
44.90 |
0.26 |
0.42 |
| 2 |
Ag |
317 |
317 |
0.00 |
55.00 |
0.30 |
0.47 |
| 3 |
Au |
256 |
256 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
686 |
686 |
237.31 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
144i |
144i |
33.39 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
344 |
344 |
0.00 |
15.76 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1104.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1104.5 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 M06-2X/6-311G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.945 |
1.264 |
| S2 |
0.000 |
0.945 |
-1.264 |
| S3 |
0.000 |
-0.945 |
1.264 |
| S4 |
0.000 |
-0.945 |
-1.264 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5289 | 1.8892 | 3.1567 |
S2 | 2.5289 | | 3.1567 | 1.8892 | S3 | 1.8892 | 3.1567 | | 2.5289 | S4 | 3.1567 | 1.8892 | 2.5289 | |
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 M06-2X/6-311G*
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 |
-53.034 |
0.000 |
0.000 |
| y |
0.000 |
-50.242 |
0.000 |
| z |
0.000 |
0.000 |
-55.241 |
|
| Traceless |
| | x | y | z |
| x |
-0.293 |
0.000 |
0.000 |
| y |
0.000 |
3.896 |
0.000 |
| z |
0.000 |
0.000 |
-3.604 |
|
| Polar |
| 3z2-r2 | -7.207 |
| x2-y2 | -2.792 |
| 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 |
4.559 |
0.000 |
0.000 |
| y |
0.000 |
12.183 |
0.000 |
| z |
0.000 |
0.000 |
19.179 |
<r2> (average value of r
2) Å
2
| <r2> |
192.435 |
| (<r2>)1/2 |
13.872 |