Jump to
S1C2
S1C3
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.651349 |
| Energy at 298.15K | |
| HF Energy | -1584.651349 |
| Nuclear repulsion energy | 317.512712 |
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 B3PW91/3-21G
| 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 |
456 |
439 |
0.00 |
|
|
|
| 2 |
A1 |
153 |
147 |
0.00 |
|
|
|
| 3 |
B1 |
359 |
345 |
0.00 |
|
|
|
| 4 |
B2 |
262 |
252 |
0.23 |
|
|
|
| 5 |
E |
358 |
344 |
0.05 |
|
|
|
| 5 |
E |
358 |
344 |
0.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 972.7 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 935.0 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 B3PW91/3-21G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.573 |
0.366 |
| S2 |
0.000 |
-1.573 |
0.366 |
| S3 |
-1.573 |
0.000 |
-0.366 |
| S4 |
1.573 |
0.000 |
-0.366 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.1459 | 2.3418 | 2.3418 |
S2 | 3.1459 | | 2.3418 | 2.3418 | S3 | 2.3418 | 2.3418 | | 3.1459 | S4 | 2.3418 | 2.3418 | 3.1459 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.803 |
|
S1 |
S3 |
S4 |
47.803 |
| S2 |
S1 |
S3 |
47.803 |
|
S2 |
S4 |
S3 |
47.803 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
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 |
-51.855 |
0.000 |
0.000 |
| y |
0.000 |
-51.855 |
0.000 |
| z |
0.000 |
0.000 |
-56.703 |
|
| Traceless |
| | x | y | z |
| x |
2.424 |
0.000 |
0.000 |
| y |
0.000 |
2.424 |
0.000 |
| z |
0.000 |
0.000 |
-4.848 |
|
| Polar |
| 3z2-r2 | -9.697 |
| 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 |
12.398 |
0.000 |
0.000 |
| y |
0.000 |
12.398 |
0.000 |
| z |
0.000 |
0.000 |
4.231 |
<r2> (average value of r
2) Å
2
| <r2> |
200.320 |
| (<r2>)1/2 |
14.153 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.668283 |
| Energy at 298.15K | |
| HF Energy | -1584.668283 |
| Nuclear repulsion energy | 310.855715 |
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 B3PW91/3-21G
| 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 |
577 |
554 |
0.00 |
|
|
|
| 2 |
A1 |
299 |
287 |
0.00 |
|
|
|
| 3 |
A1 |
110 |
106 |
8.18 |
|
|
|
| 4 |
A2 |
199 |
192 |
0.00 |
|
|
|
| 5 |
B2 |
542 |
521 |
75.24 |
|
|
|
| 6 |
B2 |
275 |
265 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1001.4 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 962.5 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 B3PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.351 |
1.034 |
| S2 |
0.000 |
-1.351 |
1.034 |
| S3 |
0.000 |
1.352 |
-1.034 |
| S4 |
0.000 |
-1.352 |
-1.034 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7029 | 2.0680 | 3.4034 |
S2 | 2.7029 | | 3.4034 | 2.0680 | S3 | 2.0680 | 3.4034 | | 2.7035 | S4 | 3.4034 | 2.0680 | 2.7035 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.008 |
|
S1 |
S3 |
S4 |
89.992 |
| S2 |
S1 |
S3 |
90.008 |
|
S2 |
S4 |
S3 |
89.992 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/3-21G
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 |
0.001 |
0.001 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-53.380 |
0.000 |
0.000 |
| y |
0.000 |
-55.376 |
0.000 |
| z |
0.000 |
0.000 |
-52.112 |
|
| Traceless |
| | x | y | z |
| x |
0.364 |
0.000 |
0.000 |
| y |
0.000 |
-2.630 |
0.000 |
| z |
0.000 |
0.000 |
2.266 |
|
| Polar |
| 3z2-r2 | 4.532 |
| x2-y2 | 1.996 |
| 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 |
2.806 |
0.000 |
0.000 |
| y |
0.000 |
16.777 |
0.000 |
| z |
0.000 |
0.000 |
13.087 |
<r2> (average value of r
2) Å
2
| <r2> |
218.827 |
| (<r2>)1/2 |
14.793 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.668283 |
| Energy at 298.15K | |
| HF Energy | -1584.668283 |
| Nuclear repulsion energy | 310.870643 |
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 B3PW91/3-21G
| 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 |
577 |
554 |
0.00 |
|
|
|
| 2 |
Ag |
299 |
287 |
0.00 |
|
|
|
| 3 |
Au |
199 |
192 |
0.00 |
|
|
|
| 4 |
B1u |
542 |
521 |
75.26 |
|
|
|
| 5 |
B2u |
111 |
106 |
8.19 |
|
|
|
| 6 |
B3g |
275 |
265 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1001.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 962.7 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 B3PW91/3-21G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.034 |
1.352 |
| S2 |
0.000 |
1.034 |
-1.352 |
| S3 |
0.000 |
-1.034 |
1.352 |
| S4 |
0.000 |
-1.034 |
-1.352 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7030 | 2.0679 | 3.4033 |
S2 | 2.7030 | | 3.4033 | 2.0679 | S3 | 2.0679 | 3.4033 | | 2.7030 | S4 | 3.4033 | 2.0679 | 2.7030 | |
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 B3PW91/3-21G
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 |
-53.380 |
0.000 |
0.000 |
| y |
0.000 |
-52.113 |
0.000 |
| z |
0.000 |
0.000 |
-55.377 |
|
| Traceless |
| | x | y | z |
| x |
0.365 |
0.000 |
0.000 |
| y |
0.000 |
2.266 |
0.000 |
| z |
0.000 |
0.000 |
-2.630 |
|
| Polar |
| 3z2-r2 | -5.261 |
| x2-y2 | -1.267 |
| 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 |
2.806 |
0.000 |
0.000 |
| y |
0.000 |
13.086 |
0.000 |
| z |
0.000 |
0.000 |
16.775 |
<r2> (average value of r
2) Å
2
| <r2> |
218.809 |
| (<r2>)1/2 |
14.792 |