Jump to
S1C2
S1C3
Energy calculated at B3PW91/cc-pV(T+d)Z
| | hartrees |
| Energy at 0K | -1592.674540 |
| Energy at 298.15K | |
| HF Energy | -1592.674540 |
| Nuclear repulsion energy | 352.267465 |
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/cc-pV(T+d)Z
| 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 |
531 |
512 |
0.00 |
|
|
|
| 2 |
A1 |
206 |
199 |
0.00 |
|
|
|
| 3 |
B1 |
469 |
452 |
0.00 |
|
|
|
| 4 |
B2 |
298 |
288 |
0.00 |
|
|
|
| 5 |
E |
439 |
424 |
0.00 |
|
|
|
| 5 |
E |
439 |
424 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1191.4 cm
-1
Scaled (by 0.964) Zero Point Vibrational Energy (zpe) 1148.5 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/cc-pV(T+d)Z
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.423 |
0.312 |
| S2 |
0.000 |
-1.423 |
0.312 |
| S3 |
-1.423 |
0.000 |
-0.312 |
| S4 |
1.423 |
0.000 |
-0.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8470 | 2.1076 | 2.1076 |
S2 | 2.8470 | | 2.1076 | 2.1076 | S3 | 2.1076 | 2.1076 | | 2.8470 | S4 | 2.1076 | 2.1076 | 2.8470 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.515 |
|
S1 |
S3 |
S4 |
47.515 |
| S2 |
S1 |
S3 |
47.515 |
|
S2 |
S4 |
S3 |
47.515 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pV(T+d)Z
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 |
-48.529 |
0.000 |
0.000 |
| y |
0.000 |
-48.529 |
0.000 |
| z |
0.000 |
0.000 |
-53.974 |
|
| Traceless |
| | x | y | z |
| x |
2.723 |
0.000 |
0.000 |
| y |
0.000 |
2.723 |
0.000 |
| z |
0.000 |
0.000 |
-5.445 |
|
| Polar |
| 3z2-r2 | -10.891 |
| 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 |
11.324 |
0.000 |
0.000 |
| y |
0.000 |
11.324 |
0.000 |
| z |
0.000 |
0.000 |
6.639 |
<r2> (average value of r
2) Å
2
| <r2> |
167.362 |
| (<r2>)1/2 |
12.937 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/cc-pV(T+d)Z
| | hartrees |
| Energy at 0K | -1592.702645 |
| Energy at 298.15K | |
| HF Energy | -1592.702645 |
| Nuclear repulsion energy | 333.902121 |
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/cc-pV(T+d)Z
| 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 |
700 |
675 |
6.97 |
|
|
|
| 2 |
A1 |
397 |
382 |
4.97 |
|
|
|
| 3 |
A1 |
111 |
107 |
0.30 |
|
|
|
| 4 |
A2 |
219 |
211 |
0.00 |
|
|
|
| 5 |
B2 |
671 |
647 |
118.75 |
|
|
|
| 6 |
B2 |
342 |
329 |
0.18 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1219.9 cm
-1
Scaled (by 0.964) Zero Point Vibrational Energy (zpe) 1175.9 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/cc-pV(T+d)Z
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.046 |
0.909 |
| S2 |
0.000 |
-1.046 |
0.909 |
| S3 |
0.000 |
1.602 |
-0.909 |
| S4 |
0.000 |
-1.602 |
-0.909 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0921 | 1.9011 | 3.2120 |
S2 | 2.0921 | | 3.2120 | 1.9011 | S3 | 1.9011 | 3.2120 | | 3.2039 | S4 | 3.2120 | 1.9011 | 3.2039 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.001 |
|
S1 |
S3 |
S4 |
72.999 |
| S2 |
S1 |
S3 |
107.001 |
|
S2 |
S4 |
S3 |
72.999 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/cc-pV(T+d)Z
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.134 |
|
|
|
| 2 |
S |
0.134 |
|
|
|
| 3 |
S |
-0.134 |
|
|
|
| 4 |
S |
-0.134 |
|
|
|
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 |
1.391 |
1.391 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.890 |
0.000 |
0.000 |
| y |
0.000 |
-52.860 |
0.000 |
| z |
0.000 |
0.000 |
-48.262 |
|
| Traceless |
| | x | y | z |
| x |
-0.329 |
0.000 |
0.000 |
| y |
0.000 |
-3.284 |
0.000 |
| z |
0.000 |
0.000 |
3.614 |
|
| Polar |
| 3z2-r2 | 7.227 |
| x2-y2 | 1.970 |
| 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 |
5.806 |
0.000 |
0.000 |
| y |
0.000 |
18.197 |
0.000 |
| z |
0.000 |
0.000 |
11.810 |
<r2> (average value of r
2) Å
2
| <r2> |
201.666 |
| (<r2>)1/2 |
14.201 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/cc-pV(T+d)Z
| | hartrees |
| Energy at 0K | -1592.696352 |
| Energy at 298.15K | |
| HF Energy | -1592.696352 |
| Nuclear repulsion energy | 338.206711 |
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/cc-pV(T+d)Z
| 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 |
749 |
722 |
0.00 |
|
|
|
| 2 |
Ag |
300 |
289 |
0.00 |
|
|
|
| 3 |
Au |
257 |
247 |
0.00 |
|
|
|
| 4 |
B1u |
690 |
665 |
120.75 |
|
|
|
| 5 |
B2u |
155i |
149i |
16.59 |
|
|
|
| 6 |
B3g |
347 |
335 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1094.2 cm
-1
Scaled (by 0.964) Zero Point Vibrational Energy (zpe) 1054.9 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/cc-pV(T+d)Z
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.942 |
1.254 |
| S2 |
0.000 |
0.942 |
-1.254 |
| S3 |
0.000 |
-0.942 |
1.254 |
| S4 |
0.000 |
-0.942 |
-1.254 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5085 | 1.8837 | 3.1370 |
S2 | 2.5085 | | 3.1370 | 1.8837 | S3 | 1.8837 | 3.1370 | | 2.5085 | S4 | 3.1370 | 1.8837 | 2.5085 | |
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/cc-pV(T+d)Z
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 |
-51.234 |
0.000 |
0.000 |
| y |
0.000 |
-47.533 |
0.000 |
| z |
0.000 |
0.000 |
-52.501 |
|
| Traceless |
| | x | y | z |
| x |
-1.216 |
0.000 |
0.000 |
| y |
0.000 |
4.334 |
0.000 |
| z |
0.000 |
0.000 |
-3.118 |
|
| Polar |
| 3z2-r2 | -6.236 |
| x2-y2 | -3.701 |
| 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 |
5.784 |
0.000 |
0.000 |
| y |
0.000 |
12.333 |
0.000 |
| z |
0.000 |
0.000 |
17.161 |
<r2> (average value of r
2) Å
2
| <r2> |
188.950 |
| (<r2>)1/2 |
13.746 |