Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-31G
| | hartrees |
| Energy at 0K | -1592.439358 |
| Energy at 298.15K | |
| HF Energy | -1592.439358 |
| Nuclear repulsion energy | 323.407728 |
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/6-31G
| 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 |
463 |
463 |
0.00 |
62.04 |
0.07 |
0.13 |
| 2 |
A1 |
152 |
152 |
0.00 |
7.75 |
0.75 |
0.85 |
| 3 |
B1 |
392 |
392 |
0.00 |
37.36 |
0.75 |
0.86 |
| 4 |
B2 |
283 |
283 |
0.38 |
14.18 |
0.75 |
0.86 |
| 5 |
E |
380 |
380 |
0.02 |
10.81 |
0.75 |
0.86 |
| 5 |
E |
380 |
380 |
0.02 |
10.81 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1024.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1024.8 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/6-31G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.551 |
0.340 |
| S2 |
0.000 |
-1.551 |
0.340 |
| S3 |
-1.551 |
0.000 |
-0.340 |
| S4 |
1.551 |
0.000 |
-0.340 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.1012 | 2.2957 | 2.2957 |
S2 | 3.1012 | | 2.2957 | 2.2957 | S3 | 2.2957 | 2.2957 | | 3.1012 | S4 | 2.2957 | 2.2957 | 3.1012 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.512 |
|
S1 |
S3 |
S4 |
47.512 |
| S2 |
S1 |
S3 |
47.512 |
|
S2 |
S4 |
S3 |
47.512 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G
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 |
-52.075 |
0.000 |
0.000 |
| y |
0.000 |
-52.075 |
0.000 |
| z |
0.000 |
0.000 |
-56.519 |
|
| Traceless |
| | x | y | z |
| x |
2.222 |
0.000 |
0.000 |
| y |
0.000 |
2.222 |
0.000 |
| z |
0.000 |
0.000 |
-4.444 |
|
| Polar |
| 3z2-r2 | -8.888 |
| 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 |
12.679 |
0.000 |
0.000 |
| y |
0.000 |
12.679 |
0.000 |
| z |
0.000 |
0.000 |
4.602 |
<r2> (average value of r
2) Å
2
| <r2> |
194.712 |
| (<r2>)1/2 |
13.954 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-31G
| | hartrees |
| Energy at 0K | -1592.434015 |
| Energy at 298.15K | |
| HF Energy | -1592.434015 |
| Nuclear repulsion energy | 312.504859 |
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/6-31G
| 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 |
575 |
575 |
0.07 |
40.24 |
0.20 |
0.34 |
| 2 |
A1 |
346 |
346 |
3.69 |
41.30 |
0.24 |
0.39 |
| 3 |
A1 |
118 |
118 |
1.74 |
16.85 |
0.47 |
0.64 |
| 4 |
A2 |
177 |
177 |
0.00 |
0.28 |
0.75 |
0.86 |
| 5 |
B2 |
562 |
562 |
109.30 |
2.70 |
0.75 |
0.86 |
| 6 |
B2 |
275 |
275 |
0.01 |
20.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1026.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1026.9 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/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.144 |
1.001 |
| S2 |
0.000 |
-1.144 |
1.001 |
| S3 |
0.000 |
1.613 |
-1.001 |
| S4 |
0.000 |
-1.613 |
-1.001 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.2873 | 2.0564 | 3.4069 |
S2 | 2.2873 | | 3.4069 | 2.0564 | S3 | 2.0564 | 3.4069 | | 3.2256 | S4 | 3.4069 | 2.0564 | 3.2256 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
103.187 |
|
S1 |
S3 |
S4 |
76.813 |
| S2 |
S1 |
S3 |
103.187 |
|
S2 |
S4 |
S3 |
76.813 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.048 |
|
|
|
| 2 |
S |
0.048 |
|
|
|
| 3 |
S |
-0.048 |
|
|
|
| 4 |
S |
-0.048 |
|
|
|
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 |
1.255 |
1.255 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.988 |
0.000 |
0.000 |
| y |
0.000 |
-56.318 |
0.000 |
| z |
0.000 |
0.000 |
-52.866 |
|
| Traceless |
| | x | y | z |
| x |
1.603 |
0.000 |
0.000 |
| y |
0.000 |
-3.391 |
0.000 |
| z |
0.000 |
0.000 |
1.788 |
|
| Polar |
| 3z2-r2 | 3.576 |
| x2-y2 | 3.330 |
| 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 |
3.342 |
0.000 |
0.000 |
| y |
0.000 |
19.900 |
0.000 |
| z |
0.000 |
0.000 |
12.718 |
<r2> (average value of r
2) Å
2
| <r2> |
222.993 |
| (<r2>)1/2 |
14.933 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-31G
| | hartrees |
| Energy at 0K | -1592.430571 |
| Energy at 298.15K | |
| HF Energy | -1592.430571 |
| Nuclear repulsion energy | 316.055765 |
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/6-31G
| 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 |
640 |
640 |
0.00 |
42.47 |
0.29 |
0.44 |
| 2 |
Ag |
299 |
299 |
0.00 |
54.41 |
0.29 |
0.45 |
| 3 |
Au |
210 |
210 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
598 |
598 |
132.82 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
152i |
152i |
15.59 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
278 |
278 |
0.00 |
22.95 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 936.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 936.3 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 M06-2X/6-31G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.015 |
1.332 |
| S2 |
0.000 |
1.015 |
-1.332 |
| S3 |
0.000 |
-1.015 |
1.332 |
| S4 |
0.000 |
-1.015 |
-1.332 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6642 | 2.0300 | 3.3494 |
S2 | 2.6642 | | 3.3494 | 2.0300 | S3 | 2.0300 | 3.3494 | | 2.6642 | S4 | 3.3494 | 2.0300 | 2.6642 | |
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/6-31G
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 |
-53.164 |
0.000 |
0.000 |
| y |
0.000 |
-52.656 |
0.000 |
| z |
0.000 |
0.000 |
-55.837 |
|
| Traceless |
| | x | y | z |
| x |
1.083 |
0.000 |
0.000 |
| y |
0.000 |
1.844 |
0.000 |
| z |
0.000 |
0.000 |
-2.927 |
|
| Polar |
| 3z2-r2 | -5.855 |
| x2-y2 | -0.507 |
| 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 |
3.327 |
0.000 |
0.000 |
| y |
0.000 |
13.199 |
0.000 |
| z |
0.000 |
0.000 |
18.601 |
<r2> (average value of r
2) Å
2
| <r2> |
213.156 |
| (<r2>)1/2 |
14.600 |