Jump to
S1C2
S1C3
Energy calculated at B3LYP/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.869242 |
| Energy at 298.15K | |
| HF Energy | -1592.869242 |
| Nuclear repulsion energy | 346.691008 |
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/daug-cc-pVTZ
| 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 |
504 |
504 |
0.00 |
43.93 |
0.05 |
0.09 |
| 2 |
A1 |
196 |
196 |
0.00 |
1.19 |
0.74 |
0.85 |
| 3 |
B1 |
441 |
441 |
0.00 |
18.53 |
0.75 |
0.86 |
| 4 |
B2 |
298 |
298 |
0.03 |
7.48 |
0.75 |
0.86 |
| 5 |
E |
415 |
415 |
0.02 |
3.22 |
0.75 |
0.86 |
| 5 |
E |
415 |
415 |
0.02 |
3.22 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1134.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1134.3 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/daug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.448 |
0.312 |
| S2 |
0.000 |
-1.448 |
0.312 |
| S3 |
-1.448 |
0.000 |
-0.312 |
| S4 |
1.448 |
0.000 |
-0.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8961 | 2.1406 | 2.1406 |
S2 | 2.8961 | | 2.1406 | 2.1406 | S3 | 2.1406 | 2.1406 | | 2.8961 | S4 | 2.1406 | 2.1406 | 2.8961 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.433 |
|
S1 |
S3 |
S4 |
47.433 |
| S2 |
S1 |
S3 |
47.433 |
|
S2 |
S4 |
S3 |
47.433 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVTZ
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 |
-49.304 |
0.000 |
0.000 |
| y |
0.000 |
-49.304 |
0.000 |
| z |
0.000 |
0.000 |
-54.760 |
|
| Traceless |
| | x | y | z |
| x |
2.728 |
0.000 |
0.000 |
| y |
0.000 |
2.728 |
0.000 |
| z |
0.000 |
0.000 |
-5.457 |
|
| Polar |
| 3z2-r2 | -10.913 |
| 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 |
13.229 |
0.000 |
0.000 |
| y |
0.000 |
13.229 |
0.000 |
| z |
0.000 |
0.000 |
9.254 |
<r2> (average value of r
2) Å
2
| <r2> |
172.346 |
| (<r2>)1/2 |
13.128 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.897446 |
| Energy at 298.15K | |
| HF Energy | -1592.897446 |
| Nuclear repulsion energy | 328.617063 |
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/daug-cc-pVTZ
| 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 |
667 |
667 |
5.86 |
31.82 |
0.06 |
0.12 |
| 2 |
A1 |
361 |
361 |
4.93 |
37.95 |
0.14 |
0.25 |
| 3 |
A1 |
107 |
107 |
0.34 |
11.53 |
0.39 |
0.56 |
| 4 |
A2 |
207 |
207 |
0.00 |
0.12 |
0.75 |
0.86 |
| 5 |
B2 |
642 |
642 |
120.15 |
4.06 |
0.75 |
0.86 |
| 6 |
B2 |
328 |
328 |
0.16 |
8.27 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1156.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1156.1 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/daug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.069 |
0.920 |
| S2 |
0.000 |
-1.069 |
0.920 |
| S3 |
0.000 |
1.632 |
-0.920 |
| S4 |
0.000 |
-1.632 |
-0.920 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1381 | 1.9235 | 3.2680 |
S2 | 2.1381 | | 3.2680 | 1.9235 | S3 | 1.9235 | 3.2680 | | 3.2646 | S4 | 3.2680 | 1.9235 | 3.2646 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.026 |
|
S1 |
S3 |
S4 |
72.974 |
| S2 |
S1 |
S3 |
107.026 |
|
S2 |
S4 |
S3 |
72.974 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.286 |
|
|
|
| 2 |
S |
0.286 |
|
|
|
| 3 |
S |
-0.286 |
|
|
|
| 4 |
S |
-0.286 |
|
|
|
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 |
1.334 |
1.334 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.731 |
0.000 |
0.000 |
| y |
0.000 |
-53.610 |
0.000 |
| z |
0.000 |
0.000 |
-49.069 |
|
| Traceless |
| | x | y | z |
| x |
-0.392 |
0.000 |
0.000 |
| y |
0.000 |
-3.210 |
0.000 |
| z |
0.000 |
0.000 |
3.601 |
|
| Polar |
| 3z2-r2 | 7.203 |
| x2-y2 | 1.879 |
| 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 |
8.461 |
0.000 |
0.000 |
| y |
0.000 |
20.760 |
0.000 |
| z |
0.000 |
0.000 |
13.543 |
<r2> (average value of r
2) Å
2
| <r2> |
208.102 |
| (<r2>)1/2 |
14.426 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/daug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.892078 |
| Energy at 298.15K | |
| HF Energy | -1592.892078 |
| Nuclear repulsion energy | 332.458771 |
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/daug-cc-pVTZ
| 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 |
717 |
0.00 |
36.74 |
0.09 |
0.17 |
| 2 |
Ag |
282 |
282 |
0.00 |
33.70 |
0.17 |
0.30 |
| 3 |
Au |
242 |
242 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
663 |
663 |
123.46 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
139i |
139i |
14.09 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
331 |
331 |
0.00 |
8.92 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1047.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1047.5 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/daug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.953 |
1.284 |
| S2 |
0.000 |
0.953 |
-1.284 |
| S3 |
0.000 |
-0.953 |
1.284 |
| S4 |
0.000 |
-0.953 |
-1.284 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5677 | 1.9053 | 3.1974 |
S2 | 2.5677 | | 3.1974 | 1.9053 | S3 | 1.9053 | 3.1974 | | 2.5677 | S4 | 3.1974 | 1.9053 | 2.5677 | |
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/daug-cc-pVTZ
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 |
-51.953 |
0.000 |
0.000 |
| y |
0.000 |
-48.329 |
0.000 |
| z |
0.000 |
0.000 |
-53.229 |
|
| Traceless |
| | x | y | z |
| x |
-1.174 |
0.000 |
0.000 |
| y |
0.000 |
4.262 |
0.000 |
| z |
0.000 |
0.000 |
-3.088 |
|
| Polar |
| 3z2-r2 | -6.176 |
| x2-y2 | -3.624 |
| 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 |
8.440 |
0.000 |
0.000 |
| y |
0.000 |
13.969 |
0.000 |
| z |
0.000 |
0.000 |
19.604 |
<r2> (average value of r
2) Å
2
| <r2> |
195.530 |
| (<r2>)1/2 |
13.983 |