Jump to
S1C2
S1C3
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -1592.623954 |
| Energy at 298.15K | |
| HF Energy | -1592.623954 |
| Nuclear repulsion energy | 348.516548 |
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 wB97X-D/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 |
531 |
505 |
0.00 |
51.73 |
0.07 |
0.13 |
| 2 |
A1 |
198 |
188 |
0.00 |
0.85 |
0.65 |
0.79 |
| 3 |
B1 |
475 |
453 |
0.00 |
36.19 |
0.75 |
0.86 |
| 4 |
B2 |
320 |
305 |
0.21 |
8.11 |
0.75 |
0.86 |
| 5 |
E |
455 |
433 |
0.00 |
5.74 |
0.75 |
0.86 |
| 5 |
E |
455 |
433 |
0.00 |
5.74 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1217.0 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 1158.9 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 wB97X-D/6-31+G**
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.442 |
0.307 |
| S2 |
0.000 |
-1.442 |
0.307 |
| S3 |
-1.442 |
0.000 |
-0.307 |
| S4 |
1.442 |
0.000 |
-0.307 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8831 | 2.1288 | 2.1288 |
S2 | 2.8831 | | 2.1288 | 2.1288 | S3 | 2.1288 | 2.1288 | | 2.8831 | S4 | 2.1288 | 2.1288 | 2.8831 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.379 |
|
S1 |
S3 |
S4 |
47.379 |
| S2 |
S1 |
S3 |
47.379 |
|
S2 |
S4 |
S3 |
47.379 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/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 |
-49.770 |
0.000 |
0.000 |
| y |
0.000 |
-49.770 |
0.000 |
| z |
0.000 |
0.000 |
-55.318 |
|
| Traceless |
| | x | y | z |
| x |
2.774 |
0.000 |
0.000 |
| y |
0.000 |
2.774 |
0.000 |
| z |
0.000 |
0.000 |
-5.548 |
|
| Polar |
| 3z2-r2 | -11.097 |
| 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 |
11.067 |
0.000 |
0.000 |
| y |
0.000 |
11.067 |
0.000 |
| z |
0.000 |
0.000 |
7.524 |
<r2> (average value of r
2) Å
2
| <r2> |
171.249 |
| (<r2>)1/2 |
13.086 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -1592.637923 |
| Energy at 298.15K | |
| HF Energy | -1592.637923 |
| Nuclear repulsion energy | 331.688347 |
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 wB97X-D/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 |
679 |
647 |
4.05 |
35.79 |
0.11 |
0.20 |
| 2 |
A1 |
421 |
401 |
7.55 |
46.34 |
0.19 |
0.32 |
| 3 |
A1 |
130 |
124 |
0.81 |
16.07 |
0.47 |
0.64 |
| 4 |
A2 |
214 |
204 |
0.00 |
1.28 |
0.75 |
0.86 |
| 5 |
B2 |
651 |
620 |
176.17 |
4.72 |
0.75 |
0.86 |
| 6 |
B2 |
343 |
327 |
0.26 |
12.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1219.8 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 1161.6 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 wB97X-D/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.052 |
0.919 |
| S2 |
0.000 |
-1.052 |
0.919 |
| S3 |
0.000 |
1.604 |
-0.919 |
| S4 |
0.000 |
-1.604 |
-0.919 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1037 | 1.9192 | 3.2298 |
S2 | 2.1037 | | 3.2298 | 1.9192 | S3 | 1.9192 | 3.2298 | | 3.2077 | S4 | 3.2298 | 1.9192 | 3.2077 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.716 |
|
S1 |
S3 |
S4 |
73.284 |
| S2 |
S1 |
S3 |
106.716 |
|
S2 |
S4 |
S3 |
73.284 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.138 |
|
|
|
| 2 |
S |
0.138 |
|
|
|
| 3 |
S |
-0.138 |
|
|
|
| 4 |
S |
-0.138 |
|
|
|
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 |
1.865 |
1.865 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.606 |
0.000 |
0.000 |
| y |
0.000 |
-54.681 |
0.000 |
| z |
0.000 |
0.000 |
-50.151 |
|
| Traceless |
| | x | y | z |
| x |
0.810 |
0.000 |
0.000 |
| y |
0.000 |
-3.802 |
0.000 |
| z |
0.000 |
0.000 |
2.992 |
|
| Polar |
| 3z2-r2 | 5.984 |
| x2-y2 | 3.075 |
| 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 |
6.192 |
0.000 |
0.000 |
| y |
0.000 |
19.960 |
0.000 |
| z |
0.000 |
0.000 |
11.807 |
<r2> (average value of r
2) Å
2
| <r2> |
204.348 |
| (<r2>)1/2 |
14.295 |
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/6-31+G**
| | hartrees |
| Energy at 0K | -1592.630218 |
| Energy at 298.15K | |
| HF Energy | -1592.630218 |
| Nuclear repulsion energy | 335.407524 |
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 wB97X-D/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 |
750 |
715 |
0.00 |
44.01 |
0.18 |
0.30 |
| 2 |
Ag |
301 |
287 |
0.00 |
43.89 |
0.26 |
0.41 |
| 3 |
Au |
254 |
242 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
692 |
659 |
189.54 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
169i |
161i |
28.88 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
349 |
333 |
0.00 |
14.76 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1088.3 cm
-1
Scaled (by 0.9523) Zero Point Vibrational Energy (zpe) 1036.4 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 wB97X-D/6-31+G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.948 |
1.267 |
| S2 |
0.000 |
0.948 |
-1.267 |
| S3 |
0.000 |
-0.948 |
1.267 |
| S4 |
0.000 |
-0.948 |
-1.267 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5343 | 1.8960 | 3.1651 |
S2 | 2.5343 | | 3.1651 | 1.8960 | S3 | 1.8960 | 3.1651 | | 2.5343 | S4 | 3.1651 | 1.8960 | 2.5343 | |
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 wB97X-D/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 |
-51.933 |
0.000 |
0.000 |
| y |
0.000 |
-49.413 |
0.000 |
| z |
0.000 |
0.000 |
-54.122 |
|
| Traceless |
| | x | y | z |
| x |
-0.165 |
0.000 |
0.000 |
| y |
0.000 |
3.614 |
0.000 |
| z |
0.000 |
0.000 |
-3.449 |
|
| Polar |
| 3z2-r2 | -6.897 |
| x2-y2 | -2.520 |
| 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 |
6.445 |
0.000 |
0.000 |
| y |
0.000 |
12.270 |
0.000 |
| z |
0.000 |
0.000 |
18.588 |
<r2> (average value of r
2) Å
2
| <r2> |
192.652 |
| (<r2>)1/2 |
13.880 |