Jump to
S1C2
S1C3
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.124665 |
| Energy at 298.15K | |
| HF Energy | -1592.124665 |
| Nuclear repulsion energy | 349.437915 |
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 PBEPBE/Def2TZVPP
| 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 |
508 |
502 |
0.00 |
34.93 |
0.04 |
0.08 |
| 2 |
A1 |
205 |
202 |
0.00 |
2.56 |
0.74 |
0.85 |
| 3 |
B1 |
426 |
421 |
0.00 |
16.55 |
0.75 |
0.86 |
| 4 |
B2 |
278 |
275 |
0.01 |
9.77 |
0.75 |
0.86 |
| 5 |
E |
400 |
396 |
0.16 |
3.72 |
0.75 |
0.86 |
| 5 |
E |
400 |
396 |
0.16 |
3.72 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1108.6 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 1095.2 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 PBEPBE/Def2TZVPP
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.432 |
0.324 |
| S2 |
0.000 |
-1.432 |
0.324 |
| S3 |
-1.432 |
0.000 |
-0.324 |
| S4 |
1.432 |
0.000 |
-0.324 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8640 | 2.1264 | 2.1264 |
S2 | 2.8640 | | 2.1264 | 2.1264 | S3 | 2.1264 | 2.1264 | | 2.8640 | S4 | 2.1264 | 2.1264 | 2.8640 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.667 |
|
S1 |
S3 |
S4 |
47.667 |
| S2 |
S1 |
S3 |
47.667 |
|
S2 |
S4 |
S3 |
47.667 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
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 |
-48.625 |
0.000 |
0.000 |
| y |
0.000 |
-48.625 |
0.000 |
| z |
0.000 |
0.000 |
-53.921 |
|
| Traceless |
| | x | y | z |
| x |
2.648 |
0.000 |
0.000 |
| y |
0.000 |
2.648 |
0.000 |
| z |
0.000 |
0.000 |
-5.296 |
|
| Polar |
| 3z2-r2 | -10.591 |
| 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 |
11.520 |
0.000 |
0.000 |
| y |
0.000 |
11.520 |
0.000 |
| z |
0.000 |
0.000 |
6.756 |
<r2> (average value of r
2) Å
2
| <r2> |
169.436 |
| (<r2>)1/2 |
13.017 |
Jump to
S1C1
S1C3
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.166920 |
| Energy at 298.15K | |
| HF Energy | -1592.166920 |
| Nuclear repulsion energy | 331.443329 |
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 PBEPBE/Def2TZVPP
| 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 |
685 |
677 |
3.75 |
26.58 |
0.17 |
0.30 |
| 2 |
A1 |
321 |
317 |
4.98 |
30.94 |
0.20 |
0.33 |
| 3 |
A1 |
95 |
93 |
1.70 |
5.72 |
0.48 |
0.65 |
| 4 |
A2 |
219 |
216 |
0.00 |
0.04 |
0.75 |
0.86 |
| 5 |
B2 |
656 |
648 |
88.75 |
2.20 |
0.75 |
0.86 |
| 6 |
B2 |
326 |
322 |
0.00 |
12.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1150.7 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 1136.8 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 PBEPBE/Def2TZVPP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.097 |
0.931 |
| S2 |
0.000 |
-1.097 |
0.931 |
| S3 |
0.000 |
1.537 |
-0.931 |
| S4 |
0.000 |
-1.537 |
-0.931 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1932 | 1.9134 | 3.2253 |
S2 | 2.1932 | | 3.2253 | 1.9134 | S3 | 1.9134 | 3.2253 | | 3.0739 | S4 | 3.2253 | 1.9134 | 3.0739 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
103.306 |
|
S1 |
S3 |
S4 |
76.694 |
| S2 |
S1 |
S3 |
103.306 |
|
S2 |
S4 |
S3 |
76.694 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/Def2TZVPP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.098 |
|
|
|
| 2 |
S |
0.098 |
|
|
|
| 3 |
S |
-0.098 |
|
|
|
| 4 |
S |
-0.098 |
|
|
|
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 |
1.082 |
1.082 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.091 |
0.000 |
0.000 |
| y |
0.000 |
-52.683 |
0.000 |
| z |
0.000 |
0.000 |
-47.919 |
|
| Traceless |
| | x | y | z |
| x |
-0.790 |
0.000 |
0.000 |
| y |
0.000 |
-3.178 |
0.000 |
| z |
0.000 |
0.000 |
3.968 |
|
| Polar |
| 3z2-r2 | 7.936 |
| x2-y2 | 1.592 |
| 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 |
5.783 |
0.000 |
0.000 |
| y |
0.000 |
17.683 |
0.000 |
| z |
0.000 |
0.000 |
12.222 |
<r2> (average value of r
2) Å
2
| <r2> |
201.129 |
| (<r2>)1/2 |
14.182 |
Jump to
S1C1
S1C2
Energy calculated at PBEPBE/Def2TZVPP
| | hartrees |
| Energy at 0K | -1592.165117 |
| Energy at 298.15K | |
| HF Energy | -1592.165117 |
| Nuclear repulsion energy | 334.121446 |
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 PBEPBE/Def2TZVPP
| 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 |
712 |
704 |
0.00 |
31.09 |
0.20 |
0.33 |
| 2 |
Ag |
280 |
277 |
0.00 |
29.53 |
0.23 |
0.38 |
| 3 |
Au |
243 |
240 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
665 |
657 |
87.72 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
99i |
98i |
11.99 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
330 |
326 |
0.00 |
12.53 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1065.8 cm
-1
Scaled (by 0.9879) Zero Point Vibrational Energy (zpe) 1052.9 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 PBEPBE/Def2TZVPP
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.952 |
1.272 |
| S2 |
0.000 |
0.952 |
-1.272 |
| S3 |
0.000 |
-0.952 |
1.272 |
| S4 |
0.000 |
-0.952 |
-1.272 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5434 | 1.9038 | 3.1770 |
S2 | 2.5434 | | 3.1770 | 1.9038 | S3 | 1.9038 | 3.1770 | | 2.5434 | S4 | 3.1770 | 1.9038 | 2.5434 | |
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 PBEPBE/Def2TZVPP
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 |
-51.311 |
0.000 |
0.000 |
| y |
0.000 |
-47.467 |
0.000 |
| z |
0.000 |
0.000 |
-52.477 |
|
| Traceless |
| | x | y | z |
| x |
-1.339 |
0.000 |
0.000 |
| y |
0.000 |
4.427 |
0.000 |
| z |
0.000 |
0.000 |
-3.088 |
|
| Polar |
| 3z2-r2 | -6.176 |
| x2-y2 | -3.844 |
| 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 |
5.769 |
0.000 |
0.000 |
| y |
0.000 |
12.547 |
0.000 |
| z |
0.000 |
0.000 |
17.041 |
<r2> (average value of r
2) Å
2
| <r2> |
192.985 |
| (<r2>)1/2 |
13.892 |