Jump to
S1C2
S1C3
Energy calculated at B2PLYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.310431 |
| Energy at 298.15K | |
| HF Energy | -1592.075341 |
| Nuclear repulsion energy | 348.508367 |
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 B2PLYP/aug-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 |
514 |
493 |
0.00 |
43.02 |
0.04 |
0.08 |
| 2 |
A1 |
202 |
194 |
0.00 |
1.14 |
0.72 |
0.84 |
| 3 |
B1 |
452 |
435 |
0.00 |
17.28 |
0.75 |
0.86 |
| 4 |
B2 |
301 |
289 |
0.03 |
6.98 |
0.75 |
0.86 |
| 5 |
E |
425 |
409 |
0.00 |
3.27 |
0.75 |
0.86 |
| 5 |
E |
425 |
409 |
0.00 |
3.27 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1159.1 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 1113.9 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 B2PLYP/aug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.438 |
0.317 |
| S2 |
0.000 |
-1.438 |
0.317 |
| S3 |
-1.438 |
0.000 |
-0.317 |
| S4 |
1.438 |
0.000 |
-0.317 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8768 | 2.1306 | 2.1306 |
S2 | 2.8768 | | 2.1306 | 2.1306 | S3 | 2.1306 | 2.1306 | | 2.8768 | S4 | 2.1306 | 2.1306 | 2.8768 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.538 |
|
S1 |
S3 |
S4 |
47.538 |
| S2 |
S1 |
S3 |
47.538 |
|
S2 |
S4 |
S3 |
47.538 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-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 |
-49.466 |
0.000 |
0.000 |
| y |
0.000 |
-49.437 |
0.000 |
| z |
0.000 |
0.000 |
-55.037 |
|
| Traceless |
| | x | y | z |
| x |
2.772 |
0.000 |
0.000 |
| y |
0.000 |
2.814 |
0.000 |
| z |
0.000 |
0.000 |
-5.586 |
|
| Polar |
| 3z2-r2 | -11.172 |
| x2-y2 | -0.028 |
| 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 |
12.997 |
0.000 |
0.000 |
| y |
0.000 |
12.995 |
0.000 |
| z |
0.000 |
0.000 |
9.146 |
<r2> (average value of r
2) Å
2
| <r2> |
170.890 |
| (<r2>)1/2 |
13.072 |
Jump to
S1C1
S1C3
Energy calculated at B2PLYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.348120 |
| Energy at 298.15K | |
| HF Energy | -1592.062925 |
| Nuclear repulsion energy | 329.435543 |
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 B2PLYP/aug-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 |
689 |
662 |
0.00 |
41.78 |
0.08 |
0.14 |
| 2 |
A1 |
247 |
237 |
0.00 |
7.76 |
0.70 |
0.82 |
| 3 |
A1 |
110 |
106 |
7.40 |
0.00 |
0.46 |
0.63 |
| 4 |
A2 |
230 |
221 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
671 |
645 |
38.68 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
315 |
303 |
0.00 |
7.66 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1131.1 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 1087.0 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 B2PLYP/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.300 |
0.958 |
| S2 |
0.000 |
-1.300 |
0.958 |
| S3 |
0.000 |
1.301 |
-0.958 |
| S4 |
0.000 |
-1.301 |
-0.958 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6006 | 1.9156 | 3.2309 |
S2 | 2.6006 | | 3.2309 | 1.9156 | S3 | 1.9156 | 3.2309 | | 2.6028 | S4 | 3.2309 | 1.9156 | 2.6028 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.033 |
|
S1 |
S3 |
S4 |
89.967 |
| S2 |
S1 |
S3 |
90.033 |
|
S2 |
S4 |
S3 |
89.967 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/aug-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 |
0.003 |
0.003 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.261 |
0.000 |
0.000 |
| y |
0.000 |
-53.326 |
0.000 |
| z |
0.000 |
0.000 |
-48.452 |
|
| Traceless |
| | x | y | z |
| x |
-1.372 |
0.000 |
0.000 |
| y |
0.000 |
-2.970 |
0.000 |
| z |
0.000 |
0.000 |
4.341 |
|
| Polar |
| 3z2-r2 | 8.683 |
| x2-y2 | 1.065 |
| 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 |
8.366 |
0.000 |
0.000 |
| y |
0.000 |
17.497 |
0.000 |
| z |
0.000 |
0.000 |
14.014 |
<r2> (average value of r
2) Å
2
| <r2> |
199.085 |
| (<r2>)1/2 |
14.110 |
Jump to
S1C1
S1C2
Energy calculated at B2PLYP/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.348120 |
| Energy at 298.15K | |
| HF Energy | -1592.062880 |
| Nuclear repulsion energy | 329.354586 |
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 B2PLYP/aug-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 |
688 |
662 |
0.00 |
41.79 |
0.08 |
0.14 |
| 2 |
Ag |
247 |
237 |
0.00 |
8.03 |
0.70 |
0.82 |
| 3 |
Au |
230 |
221 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
671 |
645 |
38.51 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
110 |
106 |
7.38 |
0.00 |
0.49 |
0.66 |
| 6 |
B3g |
315 |
303 |
0.00 |
7.67 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1130.4 cm
-1
Scaled (by 0.961) Zero Point Vibrational Energy (zpe) 1086.3 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 B2PLYP/aug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.958 |
1.301 |
| S2 |
0.000 |
0.958 |
-1.301 |
| S3 |
0.000 |
-0.958 |
1.301 |
| S4 |
0.000 |
-0.958 |
-1.301 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6028 | 1.9158 | 3.2318 |
S2 | 2.6028 | | 3.2318 | 1.9158 | S3 | 1.9158 | 3.2318 | | 2.6028 | S4 | 3.2318 | 1.9158 | 2.6028 | |
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 B2PLYP/aug-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 |
-52.263 |
0.000 |
0.000 |
| y |
0.000 |
-48.453 |
0.000 |
| z |
0.000 |
0.000 |
-53.322 |
|
| Traceless |
| | x | y | z |
| x |
-1.375 |
0.000 |
0.000 |
| y |
0.000 |
4.340 |
0.000 |
| z |
0.000 |
0.000 |
-2.965 |
|
| Polar |
| 3z2-r2 | -5.930 |
| x2-y2 | -3.810 |
| 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 |
8.367 |
0.000 |
0.000 |
| y |
0.000 |
14.017 |
0.000 |
| z |
0.000 |
0.000 |
17.494 |
<r2> (average value of r
2) Å
2
| <r2> |
199.184 |
| (<r2>)1/2 |
14.113 |