Jump to
S1C2
S1C3
Energy calculated at B3PW91/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.668956 |
| Energy at 298.15K | |
| HF Energy | -1592.668956 |
| Nuclear repulsion energy | 350.307915 |
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/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 |
527 |
509 |
0.00 |
40.61 |
0.04 |
0.08 |
| 2 |
A1 |
203 |
196 |
0.00 |
1.07 |
0.73 |
0.84 |
| 3 |
B1 |
464 |
448 |
0.00 |
16.64 |
0.75 |
0.86 |
| 4 |
B2 |
298 |
287 |
0.01 |
7.11 |
0.75 |
0.86 |
| 5 |
E |
437 |
422 |
0.00 |
2.99 |
0.75 |
0.86 |
| 5 |
E |
437 |
422 |
0.00 |
2.99 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1183.3 cm
-1
Scaled (by 0.9651) Zero Point Vibrational Energy (zpe) 1142.0 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 B3PW91/aug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.432 |
0.313 |
| S2 |
0.000 |
-1.432 |
0.313 |
| S3 |
-1.432 |
0.000 |
-0.313 |
| S4 |
1.432 |
0.000 |
-0.313 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8631 | 2.1194 | 2.1194 |
S2 | 2.8631 | | 2.1194 | 2.1194 | S3 | 2.1194 | 2.1194 | | 2.8631 | S4 | 2.1194 | 2.1194 | 2.8631 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.510 |
|
S1 |
S3 |
S4 |
47.510 |
| S2 |
S1 |
S3 |
47.510 |
|
S2 |
S4 |
S3 |
47.510 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/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 |
-48.774 |
0.000 |
0.000 |
| y |
0.000 |
-48.774 |
0.000 |
| z |
0.000 |
0.000 |
-54.306 |
|
| Traceless |
| | x | y | z |
| x |
2.766 |
0.000 |
0.000 |
| y |
0.000 |
2.766 |
0.000 |
| z |
0.000 |
0.000 |
-5.532 |
|
| Polar |
| 3z2-r2 | -11.064 |
| 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 |
12.764 |
0.000 |
0.000 |
| y |
0.000 |
12.764 |
0.000 |
| z |
0.000 |
0.000 |
9.008 |
<r2> (average value of r
2) Å
2
| <r2> |
169.063 |
| (<r2>)1/2 |
13.002 |
Jump to
S1C1
S1C3
Energy calculated at B3PW91/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.694471 |
| Energy at 298.15K | |
| HF Energy | -1592.694471 |
| Nuclear repulsion energy | 332.345508 |
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/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 |
692 |
667 |
6.19 |
31.29 |
0.06 |
0.12 |
| 2 |
A1 |
384 |
370 |
5.04 |
37.31 |
0.14 |
0.25 |
| 3 |
A1 |
113 |
109 |
0.48 |
10.26 |
0.38 |
0.55 |
| 4 |
A2 |
216 |
209 |
0.00 |
0.14 |
0.75 |
0.86 |
| 5 |
B2 |
664 |
641 |
116.01 |
3.77 |
0.75 |
0.86 |
| 6 |
B2 |
336 |
324 |
0.14 |
7.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1202.0 cm
-1
Scaled (by 0.9651) Zero Point Vibrational Energy (zpe) 1160.1 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 B3PW91/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.058 |
0.918 |
| S2 |
0.000 |
-1.058 |
0.918 |
| S3 |
0.000 |
1.592 |
-0.918 |
| S4 |
0.000 |
-1.592 |
-0.918 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1162 | 1.9117 | 3.2236 |
S2 | 2.1162 | | 3.2236 | 1.9117 | S3 | 1.9117 | 3.2236 | | 3.1834 | S4 | 3.2236 | 1.9117 | 3.1834 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.207 |
|
S1 |
S3 |
S4 |
73.793 |
| S2 |
S1 |
S3 |
106.207 |
|
S2 |
S4 |
S3 |
73.793 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.180 |
|
|
|
| 2 |
S |
0.180 |
|
|
|
| 3 |
S |
-0.180 |
|
|
|
| 4 |
S |
-0.180 |
|
|
|
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 |
1.320 |
1.320 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.299 |
0.000 |
0.000 |
| y |
0.000 |
-53.020 |
0.000 |
| z |
0.000 |
0.000 |
-48.403 |
|
| Traceless |
| | x | y | z |
| x |
-0.588 |
0.000 |
0.000 |
| y |
0.000 |
-3.169 |
0.000 |
| z |
0.000 |
0.000 |
3.757 |
|
| Polar |
| 3z2-r2 | 7.513 |
| x2-y2 | 1.720 |
| 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 |
8.215 |
0.000 |
0.000 |
| y |
0.000 |
19.921 |
0.000 |
| z |
0.000 |
0.000 |
13.171 |
<r2> (average value of r
2) Å
2
| <r2> |
202.613 |
| (<r2>)1/2 |
14.234 |
Jump to
S1C1
S1C2
Energy calculated at B3PW91/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1592.689179 |
| Energy at 298.15K | |
| HF Energy | -1592.689179 |
| Nuclear repulsion energy | 336.379519 |
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/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 |
741 |
715 |
0.00 |
37.11 |
0.09 |
0.16 |
| 2 |
Ag |
300 |
289 |
0.00 |
31.65 |
0.18 |
0.30 |
| 3 |
Au |
252 |
243 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
684 |
661 |
118.26 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
146i |
141i |
15.14 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
342 |
330 |
0.00 |
8.57 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1086.1 cm
-1
Scaled (by 0.9651) Zero Point Vibrational Energy (zpe) 1048.2 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/aug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.947 |
1.261 |
| S2 |
0.000 |
0.947 |
-1.261 |
| S3 |
0.000 |
-0.947 |
1.261 |
| S4 |
0.000 |
-0.947 |
-1.261 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5218 | 1.8942 | 3.1540 |
S2 | 2.5218 | | 3.1540 | 1.8942 | S3 | 1.8942 | 3.1540 | | 2.5218 | S4 | 3.1540 | 1.8942 | 2.5218 | |
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/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 |
-51.514 |
0.000 |
0.000 |
| y |
0.000 |
-47.716 |
0.000 |
| z |
0.000 |
0.000 |
-52.728 |
|
| Traceless |
| | x | y | z |
| x |
-1.292 |
0.000 |
0.000 |
| y |
0.000 |
4.405 |
0.000 |
| z |
0.000 |
0.000 |
-3.113 |
|
| Polar |
| 3z2-r2 | -6.227 |
| x2-y2 | -3.798 |
| 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 |
8.194 |
0.000 |
0.000 |
| y |
0.000 |
13.541 |
0.000 |
| z |
0.000 |
0.000 |
18.902 |
<r2> (average value of r
2) Å
2
| <r2> |
190.798 |
| (<r2>)1/2 |
13.813 |