Jump to
S1C2
S1C3
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -1575.096933 |
| Energy at 298.15K | |
| HF Energy | -1575.096933 |
| Nuclear repulsion energy | 341.528969 |
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 B3LYP/STO-3G
| 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 |
619 |
552 |
0.00 |
24.64 |
0.09 |
0.16 |
| 2 |
A1 |
157 |
140 |
0.00 |
1.84 |
0.73 |
0.84 |
| 3 |
B1 |
563 |
502 |
0.00 |
15.30 |
0.75 |
0.86 |
| 4 |
B2 |
337 |
300 |
0.84 |
6.23 |
0.75 |
0.86 |
| 5 |
E |
551 |
492 |
1.29 |
3.37 |
0.75 |
0.86 |
| 5 |
E |
551 |
492 |
1.29 |
3.37 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1388.7 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 1239.3 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 B3LYP/STO-3G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.486 |
0.257 |
| S2 |
0.000 |
-1.486 |
0.257 |
| S3 |
-1.486 |
0.000 |
-0.257 |
| S4 |
1.486 |
0.000 |
-0.257 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9727 | 2.1642 | 2.1642 |
S2 | 2.9727 | | 2.1642 | 2.1642 | S3 | 2.1642 | 2.1642 | | 2.9727 | S4 | 2.1642 | 2.1642 | 2.9727 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
46.623 |
|
S1 |
S3 |
S4 |
46.623 |
| S2 |
S1 |
S3 |
46.623 |
|
S2 |
S4 |
S3 |
46.623 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
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 |
-43.675 |
0.000 |
0.000 |
| y |
0.000 |
-43.675 |
0.000 |
| z |
0.000 |
0.000 |
-45.778 |
|
| Traceless |
| | x | y | z |
| x |
1.052 |
0.000 |
0.000 |
| y |
0.000 |
1.052 |
0.000 |
| z |
0.000 |
0.000 |
-2.103 |
|
| Polar |
| 3z2-r2 | -4.207 |
| 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 |
6.003 |
0.000 |
0.000 |
| y |
0.000 |
6.003 |
0.000 |
| z |
0.000 |
0.000 |
0.901 |
<r2> (average value of r
2) Å
2
| <r2> |
173.349 |
| (<r2>)1/2 |
13.166 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -1575.068728 |
| Energy at 298.15K | |
| HF Energy | -1575.068728 |
| Nuclear repulsion energy | 327.105771 |
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 B3LYP/STO-3G
| 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 |
758 |
676 |
0.02 |
15.36 |
0.21 |
0.34 |
| 2 |
A1 |
371 |
331 |
4.75 |
14.45 |
0.24 |
0.39 |
| 3 |
A1 |
117 |
105 |
7.09 |
2.06 |
0.56 |
0.72 |
| 4 |
A2 |
205 |
183 |
0.00 |
0.01 |
0.75 |
0.86 |
| 5 |
B2 |
756 |
675 |
30.13 |
0.38 |
0.75 |
0.86 |
| 6 |
B2 |
332 |
296 |
0.30 |
8.92 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1269.4 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 1132.8 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 B3LYP/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.158 |
0.973 |
| S2 |
0.000 |
-1.158 |
0.973 |
| S3 |
0.000 |
1.436 |
-0.973 |
| S4 |
0.000 |
-1.436 |
-0.973 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.3165 | 1.9650 | 3.2423 |
S2 | 2.3165 | | 3.2423 | 1.9650 | S3 | 1.9650 | 3.2423 | | 2.8714 | S4 | 3.2423 | 1.9650 | 2.8714 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
98.117 |
|
S1 |
S3 |
S4 |
81.883 |
| S2 |
S1 |
S3 |
98.117 |
|
S2 |
S4 |
S3 |
81.883 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.046 |
|
|
|
| 2 |
S |
0.046 |
|
|
|
| 3 |
S |
-0.046 |
|
|
|
| 4 |
S |
-0.046 |
|
|
|
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 |
0.901 |
0.901 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-42.434 |
0.000 |
0.000 |
| y |
0.000 |
-44.741 |
0.000 |
| z |
0.000 |
0.000 |
-44.548 |
|
| Traceless |
| | x | y | z |
| x |
2.210 |
0.000 |
0.000 |
| y |
0.000 |
-1.249 |
0.000 |
| z |
0.000 |
0.000 |
-0.961 |
|
| Polar |
| 3z2-r2 | -1.922 |
| x2-y2 | 2.306 |
| 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 |
1.212 |
0.000 |
0.000 |
| y |
0.000 |
9.396 |
0.000 |
| z |
0.000 |
0.000 |
6.481 |
<r2> (average value of r
2) Å
2
| <r2> |
196.859 |
| (<r2>)1/2 |
14.031 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/STO-3G
| | hartrees |
| Energy at 0K | -1575.068003 |
| Energy at 298.15K | |
| HF Energy | -1575.068003 |
| Nuclear repulsion energy | 328.568231 |
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 B3LYP/STO-3G
| 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 |
792 |
706 |
0.00 |
15.59 |
0.23 |
0.37 |
| 2 |
Ag |
364 |
325 |
0.00 |
15.89 |
0.26 |
0.41 |
| 3 |
Au |
222 |
198 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
776 |
692 |
34.21 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
97i |
86i |
17.44 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
336 |
300 |
0.00 |
9.12 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1195.9 cm
-1
Scaled (by 0.8924) Zero Point Vibrational Energy (zpe) 1067.3 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 B3LYP/STO-3G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.977 |
1.280 |
| S2 |
0.000 |
0.977 |
-1.280 |
| S3 |
0.000 |
-0.977 |
1.280 |
| S4 |
0.000 |
-0.977 |
-1.280 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5603 | 1.9545 | 3.2210 |
S2 | 2.5603 | | 3.2210 | 1.9545 | S3 | 1.9545 | 3.2210 | | 2.5603 | S4 | 3.2210 | 1.9545 | 2.5603 | |
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 B3LYP/STO-3G
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 |
-42.437 |
0.000 |
0.000 |
| y |
0.000 |
-44.482 |
0.000 |
| z |
0.000 |
0.000 |
-44.164 |
|
| Traceless |
| | x | y | z |
| x |
1.886 |
0.000 |
0.000 |
| y |
0.000 |
-1.182 |
0.000 |
| z |
0.000 |
0.000 |
-0.704 |
|
| Polar |
| 3z2-r2 | -1.409 |
| x2-y2 | 2.045 |
| 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 |
1.199 |
0.000 |
0.000 |
| y |
0.000 |
6.621 |
0.000 |
| z |
0.000 |
0.000 |
9.139 |
<r2> (average value of r
2) Å
2
| <r2> |
193.287 |
| (<r2>)1/2 |
13.903 |