Jump to
S1C2
S1C3
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1590.151523 |
| Energy at 298.15K | |
| HF Energy | -1590.151523 |
| Nuclear repulsion energy | 352.626020 |
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 HF/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 |
573 |
521 |
0.00 |
57.30 |
0.05 |
0.10 |
| 2 |
A1 |
202 |
184 |
0.00 |
1.21 |
0.75 |
0.86 |
| 3 |
B1 |
541 |
493 |
0.00 |
21.35 |
0.75 |
0.86 |
| 4 |
B2 |
355 |
323 |
0.03 |
5.94 |
0.75 |
0.86 |
| 5 |
E |
516 |
469 |
0.27 |
4.07 |
0.75 |
0.86 |
| 5 |
E |
516 |
469 |
0.27 |
4.07 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1350.9 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 1229.9 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 HF/aug-cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.430 |
0.285 |
| S2 |
0.000 |
-1.430 |
0.285 |
| S3 |
-1.430 |
0.000 |
-0.285 |
| S4 |
1.430 |
0.000 |
-0.285 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8599 | 2.1012 | 2.1012 |
S2 | 2.8599 | | 2.1012 | 2.1012 | S3 | 2.1012 | 2.1012 | | 2.8599 | S4 | 2.1012 | 2.1012 | 2.8599 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.115 |
|
S1 |
S3 |
S4 |
47.115 |
| S2 |
S1 |
S3 |
47.115 |
|
S2 |
S4 |
S3 |
47.115 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/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 |
-49.644 |
0.000 |
0.000 |
| y |
0.000 |
-49.644 |
0.000 |
| z |
0.000 |
0.000 |
-55.491 |
|
| Traceless |
| | x | y | z |
| x |
2.924 |
0.000 |
0.000 |
| y |
0.000 |
2.924 |
0.000 |
| z |
0.000 |
0.000 |
-5.847 |
|
| Polar |
| 3z2-r2 | -11.694 |
| 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 |
12.399 |
0.000 |
0.000 |
| y |
0.000 |
12.399 |
0.000 |
| z |
0.000 |
0.000 |
8.464 |
<r2> (average value of r
2) Å
2
| <r2> |
168.296 |
| (<r2>)1/2 |
12.973 |
Jump to
S1C1
S1C3
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1590.129882 |
| Energy at 298.15K | |
| HF Energy | -1590.129882 |
| Nuclear repulsion energy | 334.755377 |
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 HF/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 |
730 |
664 |
21.10 |
18.41 |
0.68 |
0.81 |
| 2 |
A1 |
570 |
519 |
1.08 |
432.27 |
0.22 |
0.37 |
| 3 |
A1 |
138 |
126 |
0.05 |
22.85 |
0.40 |
0.57 |
| 4 |
A2 |
224 |
204 |
0.00 |
0.96 |
0.75 |
0.86 |
| 5 |
B2 |
634 |
577 |
473.85 |
1.07 |
0.75 |
0.86 |
| 6 |
B2 |
367 |
334 |
1.44 |
8.58 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1331.4 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 1212.1 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 HF/aug-cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.985 |
0.880 |
| S2 |
0.000 |
-0.985 |
0.880 |
| S3 |
0.000 |
1.713 |
-0.880 |
| S4 |
0.000 |
-1.713 |
-0.880 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 1.9691 | 1.9043 | 3.2204 |
S2 | 1.9691 | | 3.2204 | 1.9043 | S3 | 1.9043 | 3.2204 | | 3.4253 | S4 | 3.2204 | 1.9043 | 3.4253 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
112.480 |
|
S1 |
S3 |
S4 |
67.520 |
| S2 |
S1 |
S3 |
112.480 |
|
S2 |
S4 |
S3 |
67.520 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.246 |
|
|
|
| 2 |
S |
0.246 |
|
|
|
| 3 |
S |
-0.246 |
|
|
|
| 4 |
S |
-0.246 |
|
|
|
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 |
2.074 |
2.074 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.249 |
0.000 |
0.000 |
| y |
0.000 |
-55.062 |
0.000 |
| z |
0.000 |
0.000 |
-49.994 |
|
| Traceless |
| | x | y | z |
| x |
0.279 |
0.000 |
0.000 |
| y |
0.000 |
-3.941 |
0.000 |
| z |
0.000 |
0.000 |
3.661 |
|
| Polar |
| 3z2-r2 | 7.323 |
| x2-y2 | 2.814 |
| 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 |
8.214 |
0.000 |
0.000 |
| y |
0.000 |
24.669 |
0.000 |
| z |
0.000 |
0.000 |
12.487 |
<r2> (average value of r
2) Å
2
| <r2> |
207.171 |
| (<r2>)1/2 |
14.393 |
Jump to
S1C1
S1C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -1590.092077 |
| Energy at 298.15K | |
| HF Energy | -1590.092077 |
| Nuclear repulsion energy | 342.449273 |
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 HF/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 |
826 |
752 |
0.00 |
38.87 |
0.12 |
0.22 |
| 2 |
Ag |
342 |
311 |
0.00 |
1341.04 |
0.30 |
0.47 |
| 3 |
Au |
284 |
258 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
678 |
617 |
660.86 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
353i |
322i |
44.92 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
381 |
347 |
0.00 |
13.30 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1078.2 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 981.6 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 HF/aug-cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.931 |
1.238 |
| S2 |
0.000 |
0.931 |
-1.238 |
| S3 |
0.000 |
-0.931 |
1.238 |
| S4 |
0.000 |
-0.931 |
-1.238 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4765 | 1.8611 | 3.0978 |
S2 | 2.4765 | | 3.0978 | 1.8611 | S3 | 1.8611 | 3.0978 | | 2.4765 | S4 | 3.0978 | 1.8611 | 2.4765 | |
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 HF/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 |
-52.714 |
0.000 |
0.000 |
| y |
0.000 |
-48.897 |
0.000 |
| z |
0.000 |
0.000 |
-53.885 |
|
| Traceless |
| | x | y | z |
| x |
-1.323 |
0.000 |
0.000 |
| y |
0.000 |
4.402 |
0.000 |
| z |
0.000 |
0.000 |
-3.080 |
|
| Polar |
| 3z2-r2 | -6.159 |
| x2-y2 | -3.817 |
| 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 |
8.216 |
0.000 |
0.000 |
| y |
0.000 |
13.336 |
0.000 |
| z |
0.000 |
0.000 |
24.700 |
<r2> (average value of r
2) Å
2
| <r2> |
185.917 |
| (<r2>)1/2 |
13.635 |