Jump to
S1C2
S1C3
Energy calculated at B3PW91/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.650366 |
| Energy at 298.15K | |
| HF Energy | -1592.650366 |
| Nuclear repulsion energy | 352.180858 |
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 B3PW91/Def2TZVPP
| 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 |
530 |
530 |
0.00 |
37.07 |
0.05 |
0.09 |
| 2 |
A1 |
206 |
206 |
0.00 |
2.41 |
0.74 |
0.85 |
| 3 |
B1 |
469 |
469 |
0.00 |
16.37 |
0.75 |
0.86 |
| 4 |
B2 |
298 |
298 |
0.00 |
8.32 |
0.75 |
0.86 |
| 5 |
E |
439 |
439 |
0.00 |
4.05 |
0.75 |
0.86 |
| 5 |
E |
439 |
439 |
0.00 |
4.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1190.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1190.3 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 B3PW91/Def2TZVPP
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.424 |
0.313 |
| S2 |
0.000 |
-1.424 |
0.313 |
| S3 |
-1.424 |
0.000 |
-0.313 |
| S4 |
1.424 |
0.000 |
-0.313 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8474 | 2.1083 | 2.1083 |
S2 | 2.8474 | | 2.1083 | 2.1083 | S3 | 2.1083 | 2.1083 | | 2.8474 | S4 | 2.1083 | 2.1083 | 2.8474 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.524 |
|
S1 |
S3 |
S4 |
47.524 |
| S2 |
S1 |
S3 |
47.524 |
|
S2 |
S4 |
S3 |
47.524 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/Def2TZVPP
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 |
-48.472 |
0.000 |
0.000 |
| y |
0.000 |
-48.472 |
0.000 |
| z |
0.000 |
0.000 |
-53.889 |
|
| Traceless |
| | x | y | z |
| x |
2.708 |
0.000 |
0.000 |
| y |
0.000 |
2.708 |
0.000 |
| z |
0.000 |
0.000 |
-5.417 |
|
| Polar |
| 3z2-r2 | -10.834 |
| 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 |
11.291 |
0.000 |
0.000 |
| y |
0.000 |
11.291 |
0.000 |
| z |
0.000 |
0.000 |
6.581 |
<r2> (average value of r
2) Å
2
| <r2> |
167.378 |
| (<r2>)1/2 |
12.937 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.678087 |
| Energy at 298.15K | |
| HF Energy | -1592.678087 |
| Nuclear repulsion energy | 333.985439 |
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 B3PW91/Def2TZVPP
| 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 |
699 |
699 |
6.98 |
24.80 |
0.16 |
0.27 |
| 2 |
A1 |
396 |
396 |
5.07 |
38.53 |
0.19 |
0.32 |
| 3 |
A1 |
112 |
112 |
0.36 |
9.95 |
0.45 |
0.62 |
| 4 |
A2 |
219 |
219 |
0.00 |
0.10 |
0.75 |
0.86 |
| 5 |
B2 |
671 |
671 |
118.15 |
3.77 |
0.75 |
0.86 |
| 6 |
B2 |
342 |
342 |
0.17 |
11.29 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1219.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1219.3 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 B3PW91/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.047 |
0.910 |
| S2 |
0.000 |
-1.047 |
0.910 |
| S3 |
0.000 |
1.598 |
-0.910 |
| S4 |
0.000 |
-1.598 |
-0.910 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0934 | 1.9017 | 3.2102 |
S2 | 2.0934 | | 3.2102 | 1.9017 | S3 | 1.9017 | 3.2102 | | 3.1951 | S4 | 3.2102 | 1.9017 | 3.1951 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.838 |
|
S1 |
S3 |
S4 |
73.162 |
| S2 |
S1 |
S3 |
106.838 |
|
S2 |
S4 |
S3 |
73.162 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.134 |
|
|
|
| 2 |
S |
0.134 |
|
|
|
| 3 |
S |
-0.134 |
|
|
|
| 4 |
S |
-0.134 |
|
|
|
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 |
1.403 |
1.403 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.839 |
0.000 |
0.000 |
| y |
0.000 |
-52.846 |
0.000 |
| z |
0.000 |
0.000 |
-48.131 |
|
| Traceless |
| | x | y | z |
| x |
-0.350 |
0.000 |
0.000 |
| y |
0.000 |
-3.362 |
0.000 |
| z |
0.000 |
0.000 |
3.711 |
|
| Polar |
| 3z2-r2 | 7.423 |
| x2-y2 | 2.008 |
| 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 |
5.723 |
0.000 |
0.000 |
| y |
0.000 |
18.132 |
0.000 |
| z |
0.000 |
0.000 |
11.787 |
<r2> (average value of r
2) Å
2
| <r2> |
201.344 |
| (<r2>)1/2 |
14.190 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.671951 |
| Energy at 298.15K | |
| HF Energy | -1592.671951 |
| Nuclear repulsion energy | 338.189938 |
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 B3PW91/Def2TZVPP
| 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 |
749 |
749 |
0.00 |
32.30 |
0.20 |
0.34 |
| 2 |
Ag |
301 |
301 |
0.00 |
35.12 |
0.24 |
0.39 |
| 3 |
Au |
257 |
257 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
690 |
690 |
119.98 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
154i |
154i |
16.90 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
348 |
348 |
0.00 |
12.86 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1094.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1094.8 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 B3PW91/Def2TZVPP
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.942 |
1.254 |
| S2 |
0.000 |
0.942 |
-1.254 |
| S3 |
0.000 |
-0.942 |
1.254 |
| S4 |
0.000 |
-0.942 |
-1.254 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5080 | 1.8843 | 3.1369 |
S2 | 2.5080 | | 3.1369 | 1.8843 | S3 | 1.8843 | 3.1369 | | 2.5080 | S4 | 3.1369 | 1.8843 | 2.5080 | |
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 B3PW91/Def2TZVPP
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 |
-51.179 |
0.000 |
0.000 |
| y |
0.000 |
-47.421 |
0.000 |
| z |
0.000 |
0.000 |
-52.437 |
|
| Traceless |
| | x | y | z |
| x |
-1.250 |
0.000 |
0.000 |
| y |
0.000 |
4.387 |
0.000 |
| z |
0.000 |
0.000 |
-3.137 |
|
| Polar |
| 3z2-r2 | -6.275 |
| x2-y2 | -3.758 |
| 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 |
5.700 |
0.000 |
0.000 |
| y |
0.000 |
12.301 |
0.000 |
| z |
0.000 |
0.000 |
17.123 |
<r2> (average value of r
2) Å
2
| <r2> |
188.891 |
| (<r2>)1/2 |
13.744 |