Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-31+G**
| | hartrees |
| Energy at 0K | -1592.561470 |
| Energy at 298.15K | |
| HF Energy | -1592.561470 |
| Nuclear repulsion energy | 348.700725 |
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/6-31+G**
| 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 |
496 |
0.00 |
55.55 |
0.07 |
0.13 |
| 2 |
A1 |
199 |
189 |
0.00 |
0.92 |
0.63 |
0.77 |
| 3 |
B1 |
467 |
444 |
0.00 |
39.32 |
0.75 |
0.86 |
| 4 |
B2 |
325 |
310 |
0.14 |
7.99 |
0.75 |
0.86 |
| 5 |
E |
445 |
424 |
0.00 |
6.56 |
0.75 |
0.86 |
| 5 |
E |
445 |
424 |
0.00 |
6.56 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1200.7 cm
-1
Scaled (by 0.9522) Zero Point Vibrational Energy (zpe) 1143.3 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/6-31+G**
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.438 |
0.314 |
| S2 |
0.000 |
-1.438 |
0.314 |
| S3 |
-1.438 |
0.000 |
-0.314 |
| S4 |
1.438 |
0.000 |
-0.314 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8768 | 2.1290 | 2.1290 |
S2 | 2.8768 | | 2.1290 | 2.1290 | S3 | 2.1290 | 2.1290 | | 2.8768 | S4 | 2.1290 | 2.1290 | 2.8768 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.499 |
|
S1 |
S3 |
S4 |
47.499 |
| S2 |
S1 |
S3 |
47.499 |
|
S2 |
S4 |
S3 |
47.499 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31+G**
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 |
-50.127 |
0.000 |
0.000 |
| y |
0.000 |
-50.127 |
0.000 |
| z |
0.000 |
0.000 |
-55.639 |
|
| Traceless |
| | x | y | z |
| x |
2.756 |
0.000 |
0.000 |
| y |
0.000 |
2.756 |
0.000 |
| z |
0.000 |
0.000 |
-5.511 |
|
| Polar |
| 3z2-r2 | -11.022 |
| 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 |
11.246 |
0.000 |
0.000 |
| y |
0.000 |
11.246 |
0.000 |
| z |
0.000 |
0.000 |
7.584 |
<r2> (average value of r
2) Å
2
| <r2> |
171.187 |
| (<r2>)1/2 |
13.084 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-31+G**
| | hartrees |
| Energy at 0K | -1592.573904 |
| Energy at 298.15K | |
| HF Energy | -1592.573904 |
| Nuclear repulsion energy | 332.082351 |
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/6-31+G**
| 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 |
688 |
655 |
3.88 |
35.52 |
0.11 |
0.20 |
| 2 |
A1 |
407 |
387 |
7.23 |
52.74 |
0.20 |
0.33 |
| 3 |
A1 |
125 |
119 |
0.59 |
15.56 |
0.47 |
0.64 |
| 4 |
A2 |
213 |
203 |
0.00 |
1.49 |
0.75 |
0.86 |
| 5 |
B2 |
660 |
628 |
190.18 |
4.99 |
0.75 |
0.86 |
| 6 |
B2 |
337 |
321 |
0.19 |
11.71 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1214.3 cm
-1
Scaled (by 0.9522) Zero Point Vibrational Energy (zpe) 1156.2 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 M06-2X/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.047 |
0.917 |
| S2 |
0.000 |
-1.047 |
0.917 |
| S3 |
0.000 |
1.609 |
-0.917 |
| S4 |
0.000 |
-1.609 |
-0.917 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0937 | 1.9173 | 3.2269 |
S2 | 2.0937 | | 3.2269 | 1.9173 | S3 | 1.9173 | 3.2269 | | 3.2176 | S4 | 3.2269 | 1.9173 | 3.2176 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.043 |
|
S1 |
S3 |
S4 |
72.957 |
| S2 |
S1 |
S3 |
107.043 |
|
S2 |
S4 |
S3 |
72.957 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31+G**
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 |
1.854 |
1.854 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.073 |
0.000 |
0.000 |
| y |
0.000 |
-55.027 |
0.000 |
| z |
0.000 |
0.000 |
-50.558 |
|
| Traceless |
| | x | y | z |
| x |
0.719 |
0.000 |
0.000 |
| y |
0.000 |
-3.711 |
0.000 |
| z |
0.000 |
0.000 |
2.991 |
|
| Polar |
| 3z2-r2 | 5.983 |
| x2-y2 | 2.953 |
| 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 |
6.291 |
0.000 |
0.000 |
| y |
0.000 |
20.330 |
0.000 |
| z |
0.000 |
0.000 |
11.832 |
<r2> (average value of r
2) Å
2
| <r2> |
204.479 |
| (<r2>)1/2 |
14.300 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-31+G**
| | hartrees |
| Energy at 0K | -1592.567506 |
| Energy at 298.15K | |
| HF Energy | -1592.567506 |
| Nuclear repulsion energy | 335.979322 |
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/6-31+G**
| 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 |
758 |
722 |
0.00 |
43.30 |
0.18 |
0.30 |
| 2 |
Ag |
314 |
299 |
0.00 |
49.46 |
0.26 |
0.41 |
| 3 |
Au |
253 |
241 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
696 |
663 |
209.80 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
141i |
134i |
27.06 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
344 |
327 |
0.00 |
14.86 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1112.5 cm
-1
Scaled (by 0.9522) Zero Point Vibrational Energy (zpe) 1059.3 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/6-31+G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.946 |
1.265 |
| S2 |
0.000 |
0.946 |
-1.265 |
| S3 |
0.000 |
-0.946 |
1.265 |
| S4 |
0.000 |
-0.946 |
-1.265 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5298 | 1.8930 | 3.1596 |
S2 | 2.5298 | | 3.1596 | 1.8930 | S3 | 1.8930 | 3.1596 | | 2.5298 | S4 | 3.1596 | 1.8930 | 2.5298 | |
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/6-31+G**
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 |
-52.431 |
0.000 |
0.000 |
| y |
0.000 |
-49.816 |
0.000 |
| z |
0.000 |
0.000 |
-54.573 |
|
| Traceless |
| | x | y | z |
| x |
-0.236 |
0.000 |
0.000 |
| y |
0.000 |
3.686 |
0.000 |
| z |
0.000 |
0.000 |
-3.450 |
|
| Polar |
| 3z2-r2 | -6.899 |
| x2-y2 | -2.615 |
| 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 |
6.542 |
0.000 |
0.000 |
| y |
0.000 |
12.292 |
0.000 |
| z |
0.000 |
0.000 |
18.932 |
<r2> (average value of r
2) Å
2
| <r2> |
192.380 |
| (<r2>)1/2 |
13.870 |