Jump to
S1C2
S1C3
Energy calculated at wB97X-D/LANL2DZ
| | hartrees |
| Energy at 0K | -40.326607 |
| Energy at 298.15K | |
| HF Energy | -40.326607 |
| Nuclear repulsion energy | 44.691648 |
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/LANL2DZ
| 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 |
445 |
445 |
0.00 |
53.97 |
0.06 |
0.12 |
| 2 |
A1 |
151 |
151 |
0.00 |
13.75 |
0.72 |
0.84 |
| 3 |
B1 |
378 |
378 |
0.00 |
32.17 |
0.75 |
0.86 |
| 4 |
B2 |
280 |
280 |
0.29 |
16.45 |
0.75 |
0.86 |
| 5 |
E |
361 |
361 |
0.12 |
10.42 |
0.75 |
0.86 |
| 5 |
E |
361 |
361 |
0.12 |
10.42 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 988.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 988.6 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/LANL2DZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.583 |
0.329 |
| S2 |
0.000 |
-1.583 |
0.329 |
| S3 |
-1.583 |
0.000 |
-0.329 |
| S4 |
1.583 |
0.000 |
-0.329 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.1659 | 2.3334 | 2.3334 |
S2 | 3.1659 | | 2.3334 | 2.3334 | S3 | 2.3334 | 2.3334 | | 3.1659 | S4 | 2.3334 | 2.3334 | 3.1659 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.282 |
|
S1 |
S3 |
S4 |
47.282 |
| S2 |
S1 |
S3 |
47.282 |
|
S2 |
S4 |
S3 |
47.282 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/LANL2DZ
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 |
-49.765 |
0.000 |
0.000 |
| y |
0.000 |
-49.765 |
0.000 |
| z |
0.000 |
0.000 |
-53.995 |
|
| Traceless |
| | x | y | z |
| x |
2.115 |
0.000 |
0.000 |
| y |
0.000 |
2.115 |
0.000 |
| z |
0.000 |
0.000 |
-4.229 |
|
| Polar |
| 3z2-r2 | -8.459 |
| 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 |
12.739 |
0.000 |
0.000 |
| y |
0.000 |
12.739 |
0.000 |
| z |
0.000 |
0.000 |
2.565 |
<r2> (average value of r
2) Å
2
| <r2> |
94.700 |
| (<r2>)1/2 |
9.731 |
Jump to
S1C1
S1C3
Energy calculated at wB97X-D/LANL2DZ
| | hartrees |
| Energy at 0K | -40.332836 |
| Energy at 298.15K | |
| HF Energy | -40.332836 |
| Nuclear repulsion energy | 43.566366 |
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/LANL2DZ
Geometric Data calculated at wB97X-D/LANL2DZ
Point Group is D2d
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at wB97X-D/LANL2DZ
| | hartrees |
| Energy at 0K | -40.334207 |
| Energy at 298.15K | |
| HF Energy | -40.334207 |
| Nuclear repulsion energy | 43.836929 |
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/LANL2DZ
| 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 |
614 |
614 |
0.00 |
35.26 |
0.27 |
0.43 |
| 2 |
Ag |
311 |
311 |
0.00 |
36.24 |
0.27 |
0.43 |
| 3 |
Au |
205 |
205 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
578 |
578 |
107.03 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
113 |
113 |
9.76 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
289 |
289 |
0.00 |
23.68 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1055.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1055.5 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 wB97X-D/LANL2DZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.027 |
1.353 |
| S2 |
0.000 |
1.027 |
-1.353 |
| S3 |
0.000 |
-1.027 |
1.353 |
| S4 |
0.000 |
-1.027 |
-1.353 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7069 | 2.0541 | 3.3980 |
S2 | 2.7069 | | 3.3980 | 2.0541 | S3 | 2.0541 | 3.3980 | | 2.7069 | S4 | 3.3980 | 2.0541 | 2.7069 | |
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/LANL2DZ
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 |
-50.184 |
0.000 |
0.000 |
| y |
0.000 |
-49.565 |
0.000 |
| z |
0.000 |
0.000 |
-53.525 |
|
| Traceless |
| | x | y | z |
| x |
1.361 |
0.000 |
0.000 |
| y |
0.000 |
2.289 |
0.000 |
| z |
0.000 |
0.000 |
-3.650 |
|
| Polar |
| 3z2-r2 | -7.300 |
| x2-y2 | -0.619 |
| 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 |
1.639 |
0.000 |
0.000 |
| y |
0.000 |
12.931 |
0.000 |
| z |
0.000 |
0.000 |
17.151 |
<r2> (average value of r
2) Å
2
| <r2> |
101.190 |
| (<r2>)1/2 |
10.059 |