Jump to
S1C2
S1C3
Energy calculated at BLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.836174 |
| Energy at 298.15K | |
| HF Energy | -1592.836174 |
| Nuclear repulsion energy | 343.112855 |
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 BLYP/cc-pCVTZ
| 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 |
472 |
472 |
0.00 |
|
|
|
| 2 |
A1 |
190 |
190 |
0.00 |
|
|
|
| 3 |
B1 |
390 |
390 |
0.00 |
|
|
|
| 4 |
B2 |
277 |
277 |
0.02 |
|
|
|
| 5 |
E |
365 |
365 |
0.38 |
|
|
|
| 5 |
E |
365 |
365 |
0.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1029.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1029.1 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 BLYP/cc-pCVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.462 |
0.319 |
| S2 |
0.000 |
-1.462 |
0.319 |
| S3 |
-1.462 |
0.000 |
-0.319 |
| S4 |
1.462 |
0.000 |
-0.319 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9237 | 2.1637 | 2.1637 |
S2 | 2.9237 | | 2.1637 | 2.1637 | S3 | 2.1637 | 2.1637 | | 2.9237 | S4 | 2.1637 | 2.1637 | 2.9237 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.497 |
|
S1 |
S3 |
S4 |
47.497 |
| S2 |
S1 |
S3 |
47.497 |
|
S2 |
S4 |
S3 |
47.497 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pCVTZ
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 |
-48.902 |
0.000 |
0.000 |
| y |
0.000 |
-48.902 |
0.000 |
| z |
0.000 |
0.000 |
-54.352 |
|
| Traceless |
| | x | y | z |
| x |
2.725 |
0.000 |
0.000 |
| y |
0.000 |
2.725 |
0.000 |
| z |
0.000 |
0.000 |
-5.449 |
|
| Polar |
| 3z2-r2 | -10.899 |
| 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 |
11.975 |
0.000 |
0.000 |
| y |
0.000 |
11.975 |
0.000 |
| z |
0.000 |
0.000 |
6.934 |
<r2> (average value of r
2) Å
2
| <r2> |
174.966 |
| (<r2>)1/2 |
13.227 |
Jump to
S1C1
S1C3
Energy calculated at BLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.882136 |
| Energy at 298.15K | |
| HF Energy | -1592.882136 |
| Nuclear repulsion energy | 324.548642 |
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 BLYP/cc-pCVTZ
| 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 |
648 |
648 |
3.24 |
|
|
|
| 2 |
A1 |
286 |
286 |
4.83 |
|
|
|
| 3 |
A1 |
83 |
83 |
1.12 |
|
|
|
| 4 |
A2 |
202 |
202 |
0.00 |
|
|
|
| 5 |
B2 |
621 |
621 |
92.59 |
|
|
|
| 6 |
B2 |
310 |
310 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1074.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1074.9 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 BLYP/cc-pCVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.121 |
0.936 |
| S2 |
0.000 |
-1.121 |
0.936 |
| S3 |
0.000 |
1.608 |
-0.936 |
| S4 |
0.000 |
-1.608 |
-0.936 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.2421 | 1.9337 | 3.3089 |
S2 | 2.2421 | | 3.3089 | 1.9337 | S3 | 1.9337 | 3.3089 | | 3.2156 | S4 | 3.3089 | 1.9337 | 3.2156 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
104.580 |
|
S1 |
S3 |
S4 |
75.420 |
| S2 |
S1 |
S3 |
104.580 |
|
S2 |
S4 |
S3 |
75.420 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at BLYP/cc-pCVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.094 |
|
|
|
| 2 |
S |
0.094 |
|
|
|
| 3 |
S |
-0.094 |
|
|
|
| 4 |
S |
-0.094 |
|
|
|
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 |
1.091 |
1.091 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.403 |
0.000 |
0.000 |
| y |
0.000 |
-52.925 |
0.000 |
| z |
0.000 |
0.000 |
-48.470 |
|
| Traceless |
| | x | y | z |
| x |
-0.705 |
0.000 |
0.000 |
| y |
0.000 |
-2.989 |
0.000 |
| z |
0.000 |
0.000 |
3.695 |
|
| Polar |
| 3z2-r2 | 7.389 |
| x2-y2 | 1.523 |
| 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 |
6.009 |
0.000 |
0.000 |
| y |
0.000 |
18.691 |
0.000 |
| z |
0.000 |
0.000 |
12.479 |
<r2> (average value of r
2) Å
2
| <r2> |
210.782 |
| (<r2>)1/2 |
14.518 |
Jump to
S1C1
S1C2
Energy calculated at BLYP/cc-pCVTZ
| | hartrees |
| Energy at 0K | -1592.880418 |
| Energy at 298.15K | |
| HF Energy | -1592.880418 |
| Nuclear repulsion energy | 327.458487 |
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 BLYP/cc-pCVTZ
| 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 |
676 |
676 |
0.00 |
|
|
|
| 2 |
Ag |
252 |
252 |
0.00 |
|
|
|
| 3 |
Au |
226 |
226 |
0.00 |
|
|
|
| 4 |
B1u |
632 |
632 |
91.78 |
|
|
|
| 5 |
B2u |
88i |
88i |
10.36 |
|
|
|
| 6 |
B3g |
312 |
312 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1004.8 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1004.8 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 BLYP/cc-pCVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.962 |
1.312 |
| S2 |
0.000 |
0.962 |
-1.312 |
| S3 |
0.000 |
-0.962 |
1.312 |
| S4 |
0.000 |
-0.962 |
-1.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6234 | 1.9231 | 3.2528 |
S2 | 2.6234 | | 3.2528 | 1.9231 | S3 | 1.9231 | 3.2528 | | 2.6234 | S4 | 3.2528 | 1.9231 | 2.6234 | |
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 BLYP/cc-pCVTZ
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 |
-51.624 |
0.000 |
0.000 |
| y |
0.000 |
-47.952 |
0.000 |
| z |
0.000 |
0.000 |
-52.683 |
|
| Traceless |
| | x | y | z |
| x |
-1.307 |
0.000 |
0.000 |
| y |
0.000 |
4.201 |
0.000 |
| z |
0.000 |
0.000 |
-2.895 |
|
| Polar |
| 3z2-r2 | -5.789 |
| x2-y2 | -3.672 |
| 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 |
6.000 |
0.000 |
0.000 |
| y |
0.000 |
12.865 |
0.000 |
| z |
0.000 |
0.000 |
17.844 |
<r2> (average value of r
2) Å
2
| <r2> |
200.987 |
| (<r2>)1/2 |
14.177 |