Jump to
S1C2
S1C3
Energy calculated at M06-2X/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.762603 |
| Energy at 298.15K | |
| HF Energy | -1592.762603 |
| Nuclear repulsion energy | 353.200268 |
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/cc-pCVTZ
| 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 |
545 |
545 |
0.00 |
|
|
|
| 2 |
A1 |
205 |
205 |
0.00 |
|
|
|
| 3 |
B1 |
496 |
496 |
0.00 |
|
|
|
| 4 |
B2 |
308 |
308 |
0.00 |
|
|
|
| 5 |
E |
468 |
468 |
0.01 |
|
|
|
| 5 |
E |
468 |
468 |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1244.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1244.4 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 M06-2X/cc-pCVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.420 |
0.311 |
| S2 |
0.000 |
-1.420 |
0.311 |
| S3 |
-1.420 |
0.000 |
-0.311 |
| S4 |
1.420 |
0.000 |
-0.311 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8394 | 2.1021 | 2.1021 |
S2 | 2.8394 | | 2.1021 | 2.1021 | S3 | 2.1021 | 2.1021 | | 2.8394 | S4 | 2.1021 | 2.1021 | 2.8394 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.517 |
|
S1 |
S3 |
S4 |
47.517 |
| S2 |
S1 |
S3 |
47.517 |
|
S2 |
S4 |
S3 |
47.517 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/cc-pCVTZ
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 |
-48.876 |
0.000 |
0.000 |
| y |
0.000 |
-48.876 |
0.000 |
| z |
0.000 |
0.000 |
-54.313 |
|
| Traceless |
| | x | y | z |
| x |
2.719 |
0.000 |
0.000 |
| y |
0.000 |
2.719 |
0.000 |
| z |
0.000 |
0.000 |
-5.438 |
|
| Polar |
| 3z2-r2 | -10.875 |
| 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 |
11.392 |
0.000 |
0.000 |
| y |
0.000 |
11.392 |
0.000 |
| z |
0.000 |
0.000 |
6.697 |
<r2> (average value of r
2) Å
2
| <r2> |
166.857 |
| (<r2>)1/2 |
12.917 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.774415 |
| Energy at 298.15K | |
| HF Energy | -1592.774415 |
| Nuclear repulsion energy | 335.796712 |
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/cc-pCVTZ
| 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 |
709 |
709 |
9.16 |
|
|
|
| 2 |
A1 |
466 |
466 |
4.50 |
|
|
|
| 3 |
A1 |
133 |
133 |
0.10 |
|
|
|
| 4 |
A2 |
222 |
222 |
0.00 |
|
|
|
| 5 |
B2 |
673 |
673 |
172.57 |
|
|
|
| 6 |
B2 |
347 |
347 |
0.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1274.7 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1274.7 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 M06-2X/cc-pCVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.019 |
0.901 |
| S2 |
0.000 |
-1.019 |
0.901 |
| S3 |
0.000 |
1.618 |
-0.901 |
| S4 |
0.000 |
-1.618 |
-0.901 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0377 | 1.8994 | 3.1943 |
S2 | 2.0377 | | 3.1943 | 1.8994 | S3 | 1.8994 | 3.1943 | | 3.2368 | S4 | 3.1943 | 1.8994 | 3.2368 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
108.400 |
|
S1 |
S3 |
S4 |
71.600 |
| S2 |
S1 |
S3 |
108.400 |
|
S2 |
S4 |
S3 |
71.600 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.155 |
|
|
|
| 2 |
S |
0.155 |
|
|
|
| 3 |
S |
-0.155 |
|
|
|
| 4 |
S |
-0.155 |
|
|
|
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 |
1.633 |
1.633 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.296 |
0.000 |
0.000 |
| y |
0.000 |
-53.473 |
0.000 |
| z |
0.000 |
0.000 |
-48.736 |
|
| Traceless |
| | x | y | z |
| x |
-0.192 |
0.000 |
0.000 |
| y |
0.000 |
-3.458 |
0.000 |
| z |
0.000 |
0.000 |
3.649 |
|
| Polar |
| 3z2-r2 | 7.299 |
| x2-y2 | 2.177 |
| 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 |
5.935 |
0.000 |
0.000 |
| y |
0.000 |
19.202 |
0.000 |
| z |
0.000 |
0.000 |
11.696 |
<r2> (average value of r
2) Å
2
| <r2> |
200.966 |
| (<r2>)1/2 |
14.176 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.763382 |
| Energy at 298.15K | |
| HF Energy | -1592.763382 |
| Nuclear repulsion energy | 341.115786 |
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/cc-pCVTZ
| 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 |
777 |
777 |
0.00 |
|
|
|
| 2 |
Ag |
326 |
326 |
0.00 |
|
|
|
| 3 |
Au |
265 |
265 |
0.00 |
|
|
|
| 4 |
B1u |
702 |
702 |
181.72 |
|
|
|
| 5 |
B2u |
197i |
197i |
22.40 |
|
|
|
| 6 |
B3g |
356 |
356 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1114.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1114.0 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/cc-pCVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.937 |
1.239 |
| S2 |
0.000 |
0.937 |
-1.239 |
| S3 |
0.000 |
-0.937 |
1.239 |
| S4 |
0.000 |
-0.937 |
-1.239 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4785 | 1.8737 | 3.1070 |
S2 | 2.4785 | | 3.1070 | 1.8737 | S3 | 1.8737 | 3.1070 | | 2.4785 | S4 | 3.1070 | 1.8737 | 2.4785 | |
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/cc-pCVTZ
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 |
-51.717 |
0.000 |
0.000 |
| y |
0.000 |
-47.944 |
0.000 |
| z |
0.000 |
0.000 |
-52.951 |
|
| Traceless |
| | x | y | z |
| x |
-1.269 |
0.000 |
0.000 |
| y |
0.000 |
4.390 |
0.000 |
| z |
0.000 |
0.000 |
-3.121 |
|
| Polar |
| 3z2-r2 | -6.242 |
| x2-y2 | -3.772 |
| 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 |
5.913 |
0.000 |
0.000 |
| y |
0.000 |
12.299 |
0.000 |
| z |
0.000 |
0.000 |
17.857 |
<r2> (average value of r
2) Å
2
| <r2> |
186.233 |
| (<r2>)1/2 |
13.647 |