Jump to
S1C2
S1C3
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -1592.599429 |
| Energy at 298.15K | |
| HF Energy | -1592.599429 |
| Nuclear repulsion energy | 346.460963 |
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 B3PW91/6-311G*
| 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 |
503 |
485 |
0.00 |
|
|
|
| 2 |
A1 |
196 |
189 |
0.00 |
|
|
|
| 3 |
B1 |
430 |
414 |
0.00 |
|
|
|
| 4 |
B2 |
300 |
289 |
0.07 |
|
|
|
| 5 |
E |
413 |
398 |
0.15 |
|
|
|
| 5 |
E |
413 |
398 |
0.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1127.9 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 1085.8 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 B3PW91/6-311G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.446 |
0.321 |
| S2 |
0.000 |
-1.446 |
0.321 |
| S3 |
-1.446 |
0.000 |
-0.321 |
| S4 |
1.446 |
0.000 |
-0.321 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8924 | 2.1436 | 2.1436 |
S2 | 2.8924 | | 2.1436 | 2.1436 | S3 | 2.1436 | 2.1436 | | 2.8924 | S4 | 2.1436 | 2.1436 | 2.8924 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.571 |
|
S1 |
S3 |
S4 |
47.571 |
| S2 |
S1 |
S3 |
47.571 |
|
S2 |
S4 |
S3 |
47.571 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
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 |
-50.290 |
0.000 |
0.000 |
| y |
0.000 |
-50.290 |
0.000 |
| z |
0.000 |
0.000 |
-55.544 |
|
| Traceless |
| | x | y | z |
| x |
2.627 |
0.000 |
0.000 |
| y |
0.000 |
2.627 |
0.000 |
| z |
0.000 |
0.000 |
-5.253 |
|
| Polar |
| 3z2-r2 | -10.507 |
| 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 |
10.781 |
0.000 |
0.000 |
| y |
0.000 |
10.781 |
0.000 |
| z |
0.000 |
0.000 |
5.597 |
<r2> (average value of r
2) Å
2
| <r2> |
172.954 |
| (<r2>)1/2 |
13.151 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -1592.628144 |
| Energy at 298.15K | |
| HF Energy | -1592.628144 |
| Nuclear repulsion energy | 329.155949 |
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 B3PW91/6-311G*
| 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 |
673 |
648 |
2.65 |
|
|
|
| 2 |
A1 |
322 |
310 |
8.21 |
|
|
|
| 3 |
A1 |
87 |
84 |
2.36 |
|
|
|
| 4 |
A2 |
216 |
207 |
0.00 |
|
|
|
| 5 |
B2 |
645 |
621 |
149.68 |
|
|
|
| 6 |
B2 |
329 |
316 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1135.3 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 1092.9 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 B3PW91/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.098 |
0.930 |
| S2 |
0.000 |
-1.098 |
0.930 |
| S3 |
0.000 |
1.572 |
-0.930 |
| S4 |
0.000 |
-1.572 |
-0.930 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1963 | 1.9199 | 3.2542 |
S2 | 2.1963 | | 3.2542 | 1.9199 | S3 | 1.9199 | 3.2542 | | 3.1433 | S4 | 3.2542 | 1.9199 | 3.1433 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
104.277 |
|
S1 |
S3 |
S4 |
75.723 |
| S2 |
S1 |
S3 |
104.277 |
|
S2 |
S4 |
S3 |
75.723 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.113 |
|
|
|
| 2 |
S |
0.113 |
|
|
|
| 3 |
S |
-0.113 |
|
|
|
| 4 |
S |
-0.113 |
|
|
|
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 |
1.576 |
1.576 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.234 |
0.000 |
0.000 |
| y |
0.000 |
-55.164 |
0.000 |
| z |
0.000 |
0.000 |
-50.307 |
|
| Traceless |
| | x | y | z |
| x |
0.501 |
0.000 |
0.000 |
| y |
0.000 |
-3.893 |
0.000 |
| z |
0.000 |
0.000 |
3.392 |
|
| Polar |
| 3z2-r2 | 6.785 |
| x2-y2 | 2.929 |
| 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 |
4.493 |
0.000 |
0.000 |
| y |
0.000 |
18.984 |
0.000 |
| z |
0.000 |
0.000 |
11.812 |
<r2> (average value of r
2) Å
2
| <r2> |
205.856 |
| (<r2>)1/2 |
14.348 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/6-311G*
| | hartrees |
| Energy at 0K | -1592.626468 |
| Energy at 298.15K | |
| HF Energy | -1592.626468 |
| Nuclear repulsion energy | 332.263439 |
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 B3PW91/6-311G*
| 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 |
717 |
691 |
0.00 |
|
|
|
| 2 |
Ag |
287 |
276 |
0.00 |
|
|
|
| 3 |
Au |
244 |
235 |
0.00 |
|
|
|
| 4 |
B1u |
669 |
644 |
155.10 |
|
|
|
| 5 |
B2u |
88i |
84i |
23.56 |
|
|
|
| 6 |
B3g |
331 |
319 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1079.9 cm
-1
Scaled (by 0.9627) Zero Point Vibrational Energy (zpe) 1039.7 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 B3PW91/6-311G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.952 |
1.286 |
| S2 |
0.000 |
0.952 |
-1.286 |
| S3 |
0.000 |
-0.952 |
1.286 |
| S4 |
0.000 |
-0.952 |
-1.286 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5716 | 1.9048 | 3.2002 |
S2 | 2.5716 | | 3.2002 | 1.9048 | S3 | 1.9048 | 3.2002 | | 2.5716 | S4 | 3.2002 | 1.9048 | 2.5716 | |
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 B3PW91/6-311G*
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 |
-52.521 |
0.000 |
0.000 |
| y |
0.000 |
-49.731 |
0.000 |
| z |
0.000 |
0.000 |
-54.617 |
|
| Traceless |
| | x | y | z |
| x |
-0.347 |
0.000 |
0.000 |
| y |
0.000 |
3.837 |
0.000 |
| z |
0.000 |
0.000 |
-3.490 |
|
| Polar |
| 3z2-r2 | -6.981 |
| x2-y2 | -2.790 |
| 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 |
4.471 |
0.000 |
0.000 |
| y |
0.000 |
12.241 |
0.000 |
| z |
0.000 |
0.000 |
18.220 |
<r2> (average value of r
2) Å
2
| <r2> |
196.519 |
| (<r2>)1/2 |
14.019 |