Jump to
S1C2
S1C3
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -40.546397 |
| Energy at 298.15K | |
| HF Energy | -40.546397 |
| Nuclear repulsion energy | 48.214724 |
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/CEP-121G*
| 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 |
499 |
484 |
0.00 |
51.52 |
0.06 |
0.12 |
| 2 |
A1 |
191 |
185 |
0.00 |
2.10 |
0.75 |
0.86 |
| 3 |
B1 |
432 |
419 |
0.00 |
34.85 |
0.75 |
0.86 |
| 4 |
B2 |
297 |
288 |
0.04 |
10.89 |
0.75 |
0.86 |
| 5 |
E |
414 |
402 |
0.20 |
6.50 |
0.75 |
0.86 |
| 5 |
E |
414 |
402 |
0.20 |
6.50 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1123.9 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 1089.5 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 B3LYP/CEP-121G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.463 |
0.319 |
| S2 |
0.000 |
-1.463 |
0.319 |
| S3 |
-1.463 |
0.000 |
-0.319 |
| S4 |
1.463 |
0.000 |
-0.319 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9260 | 2.1652 | 2.1652 |
S2 | 2.9260 | | 2.1652 | 2.1652 | S3 | 2.1652 | 2.1652 | | 2.9260 | S4 | 2.1652 | 2.1652 | 2.9260 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.492 |
|
S1 |
S3 |
S4 |
47.492 |
| S2 |
S1 |
S3 |
47.492 |
|
S2 |
S4 |
S3 |
47.492 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
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 |
-46.278 |
0.000 |
0.000 |
| y |
0.000 |
-46.278 |
0.000 |
| z |
0.000 |
0.000 |
-51.996 |
|
| Traceless |
| | x | y | z |
| x |
2.859 |
0.000 |
0.000 |
| y |
0.000 |
2.859 |
0.000 |
| z |
0.000 |
0.000 |
-5.718 |
|
| Polar |
| 3z2-r2 | -11.436 |
| 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 |
11.271 |
0.000 |
0.000 |
| y |
0.000 |
11.271 |
0.000 |
| z |
0.000 |
0.000 |
6.340 |
<r2> (average value of r
2) Å
2
| <r2> |
83.909 |
| (<r2>)1/2 |
9.160 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -40.573692 |
| Energy at 298.15K | |
| HF Energy | -40.573692 |
| Nuclear repulsion energy | 45.634486 |
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/CEP-121G*
| 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 |
659 |
639 |
2.95 |
34.25 |
0.20 |
0.34 |
| 2 |
A1 |
337 |
326 |
7.10 |
34.62 |
0.22 |
0.36 |
| 3 |
A1 |
94 |
91 |
1.06 |
10.29 |
0.47 |
0.64 |
| 4 |
A2 |
205 |
199 |
0.00 |
0.24 |
0.75 |
0.86 |
| 5 |
B2 |
636 |
617 |
128.03 |
2.83 |
0.75 |
0.86 |
| 6 |
B2 |
317 |
308 |
0.04 |
15.18 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1124.0 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 1089.6 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 B3LYP/CEP-121G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.100 |
0.940 |
| S2 |
0.000 |
-1.100 |
0.940 |
| S3 |
0.000 |
1.617 |
-0.940 |
| S4 |
0.000 |
-1.617 |
-0.940 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1993 | 1.9491 | 3.3033 |
S2 | 2.1993 | | 3.3033 | 1.9491 | S3 | 1.9491 | 3.3033 | | 3.2341 | S4 | 3.3033 | 1.9491 | 3.2341 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
105.395 |
|
S1 |
S3 |
S4 |
74.605 |
| S2 |
S1 |
S3 |
105.395 |
|
S2 |
S4 |
S3 |
74.605 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/CEP-121G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.116 |
|
|
|
| 2 |
S |
0.116 |
|
|
|
| 3 |
S |
-0.116 |
|
|
|
| 4 |
S |
-0.116 |
|
|
|
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 |
1.482 |
1.482 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.672 |
0.000 |
0.000 |
| y |
0.000 |
-51.032 |
0.000 |
| z |
0.000 |
0.000 |
-46.118 |
|
| Traceless |
| | x | y | z |
| x |
-0.097 |
0.000 |
0.000 |
| y |
0.000 |
-3.637 |
0.000 |
| z |
0.000 |
0.000 |
3.734 |
|
| Polar |
| 3z2-r2 | 7.468 |
| x2-y2 | 2.360 |
| 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 |
5.197 |
0.000 |
0.000 |
| y |
0.000 |
18.991 |
0.000 |
| z |
0.000 |
0.000 |
11.969 |
<r2> (average value of r
2) Å
2
| <r2> |
97.436 |
| (<r2>)1/2 |
9.871 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/CEP-121G*
| | hartrees |
| Energy at 0K | -40.570826 |
| Energy at 298.15K | |
| HF Energy | -40.570826 |
| Nuclear repulsion energy | 46.151975 |
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/CEP-121G*
| 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 |
704 |
683 |
0.00 |
41.79 |
0.24 |
0.39 |
| 2 |
Ag |
278 |
269 |
0.00 |
33.77 |
0.28 |
0.44 |
| 3 |
Au |
236 |
229 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
657 |
637 |
135.74 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
107i |
103i |
18.76 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
321 |
311 |
0.00 |
16.77 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1044.8 cm
-1
Scaled (by 0.9694) Zero Point Vibrational Energy (zpe) 1012.9 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 B3LYP/CEP-121G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.967 |
1.298 |
| S2 |
0.000 |
0.967 |
-1.298 |
| S3 |
0.000 |
-0.967 |
1.298 |
| S4 |
0.000 |
-0.967 |
-1.298 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5966 | 1.9332 | 3.2372 |
S2 | 2.5966 | | 3.2372 | 1.9332 | S3 | 1.9332 | 3.2372 | | 2.5966 | S4 | 3.2372 | 1.9332 | 2.5966 | |
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/CEP-121G*
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 |
-48.966 |
0.000 |
0.000 |
| y |
0.000 |
-45.439 |
0.000 |
| z |
0.000 |
0.000 |
-50.878 |
|
| Traceless |
| | x | y | z |
| x |
-0.808 |
0.000 |
0.000 |
| y |
0.000 |
4.483 |
0.000 |
| z |
0.000 |
0.000 |
-3.675 |
|
| Polar |
| 3z2-r2 | -7.350 |
| x2-y2 | -3.528 |
| 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 |
5.190 |
0.000 |
0.000 |
| y |
0.000 |
12.447 |
0.000 |
| z |
0.000 |
0.000 |
17.971 |
<r2> (average value of r
2) Å
2
| <r2> |
93.124 |
| (<r2>)1/2 |
9.650 |