Jump to
S1C2
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -1585.424362 |
| Energy at 298.15K | |
| HF Energy | -1585.424362 |
| Nuclear repulsion energy | 349.795749 |
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 B1B95/3-21G*
| 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 |
496 |
473 |
0.00 |
47.13 |
0.06 |
0.12 |
| 2 |
A1 |
203 |
193 |
0.00 |
3.61 |
0.75 |
0.86 |
| 3 |
B1 |
422 |
403 |
0.00 |
31.51 |
0.75 |
0.86 |
| 4 |
B2 |
316 |
301 |
0.55 |
12.28 |
0.75 |
0.86 |
| 5 |
E |
403 |
385 |
0.10 |
7.35 |
0.75 |
0.86 |
| 5 |
E |
403 |
385 |
0.10 |
7.35 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1120.7 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 1070.1 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 B1B95/3-21G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.431 |
0.323 |
| S2 |
0.000 |
-1.431 |
0.323 |
| S3 |
-1.431 |
0.000 |
-0.323 |
| S4 |
1.431 |
0.000 |
-0.323 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8614 | 2.1241 | 2.1241 |
S2 | 2.8614 | | 2.1241 | 2.1241 | S3 | 2.1241 | 2.1241 | | 2.8614 | S4 | 2.1241 | 2.1241 | 2.8614 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.657 |
|
S1 |
S3 |
S4 |
47.657 |
| S2 |
S1 |
S3 |
47.657 |
|
S2 |
S4 |
S3 |
47.657 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
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 |
-50.018 |
0.000 |
0.000 |
| y |
0.000 |
-50.018 |
0.000 |
| z |
0.000 |
0.000 |
-55.097 |
|
| Traceless |
| | x | y | z |
| x |
2.539 |
0.000 |
0.000 |
| y |
0.000 |
2.539 |
0.000 |
| z |
0.000 |
0.000 |
-5.079 |
|
| Polar |
| 3z2-r2 | -10.158 |
| 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 |
9.978 |
0.000 |
0.000 |
| y |
0.000 |
9.978 |
0.000 |
| z |
0.000 |
0.000 |
4.850 |
<r2> (average value of r
2) Å
2
| <r2> |
169.989 |
| (<r2>)1/2 |
13.038 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -1585.460012 |
| Energy at 298.15K | |
| HF Energy | -1585.460012 |
| Nuclear repulsion energy | 334.098321 |
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 B1B95/3-21G*
| 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 |
716 |
684 |
2.05 |
29.19 |
0.25 |
0.39 |
| 2 |
A1 |
302 |
289 |
6.17 |
36.17 |
0.25 |
0.40 |
| 3 |
A1 |
102 |
97 |
4.12 |
3.84 |
0.64 |
0.78 |
| 4 |
A2 |
230 |
220 |
0.00 |
0.10 |
0.75 |
0.86 |
| 5 |
B2 |
683 |
652 |
132.08 |
1.69 |
0.75 |
0.86 |
| 6 |
B2 |
346 |
330 |
0.01 |
15.79 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1189.7 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 1136.0 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 B1B95/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.091 |
0.923 |
| S2 |
0.000 |
-1.091 |
0.923 |
| S3 |
0.000 |
1.523 |
-0.923 |
| S4 |
0.000 |
-1.523 |
-0.923 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1817 | 1.8965 | 3.2002 |
S2 | 2.1817 | | 3.2002 | 1.8965 | S3 | 1.8965 | 3.2002 | | 3.0457 | S4 | 3.2002 | 1.8965 | 3.0457 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
103.167 |
|
S1 |
S3 |
S4 |
76.833 |
| S2 |
S1 |
S3 |
103.167 |
|
S2 |
S4 |
S3 |
76.833 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.074 |
|
|
|
| 2 |
S |
0.074 |
|
|
|
| 3 |
S |
-0.074 |
|
|
|
| 4 |
S |
-0.074 |
|
|
|
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 |
1.274 |
1.274 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.611 |
0.000 |
0.000 |
| y |
0.000 |
-53.952 |
0.000 |
| z |
0.000 |
0.000 |
-49.804 |
|
| Traceless |
| | x | y | z |
| x |
0.267 |
0.000 |
0.000 |
| y |
0.000 |
-3.244 |
0.000 |
| z |
0.000 |
0.000 |
2.977 |
|
| Polar |
| 3z2-r2 | 5.955 |
| x2-y2 | 2.341 |
| 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 |
3.878 |
0.000 |
0.000 |
| y |
0.000 |
16.324 |
0.000 |
| z |
0.000 |
0.000 |
10.738 |
<r2> (average value of r
2) Å
2
| <r2> |
199.195 |
| (<r2>)1/2 |
14.114 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/3-21G*
| | hartrees |
| Energy at 0K | -1585.459105 |
| Energy at 298.15K | |
| HF Energy | -1585.459105 |
| Nuclear repulsion energy | 334.072164 |
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 B1B95/3-21G*
| 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 |
757 |
723 |
0.00 |
33.74 |
0.29 |
0.45 |
| 2 |
Ag |
295 |
282 |
0.00 |
33.32 |
0.28 |
0.44 |
| 3 |
Au |
250 |
239 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
705 |
673 |
146.41 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
39i |
37i |
14.94 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
341 |
326 |
0.00 |
17.36 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1154.7 cm
-1
Scaled (by 0.9549) Zero Point Vibrational Energy (zpe) 1102.6 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 B1B95/3-21G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.942 |
1.286 |
| S2 |
0.000 |
0.942 |
-1.286 |
| S3 |
0.000 |
-0.942 |
1.286 |
| S4 |
0.000 |
-0.942 |
-1.286 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5715 | 1.8850 | 3.1884 |
S2 | 2.5715 | | 3.1884 | 1.8850 | S3 | 1.8850 | 3.1884 | | 2.5715 | S4 | 3.1884 | 1.8850 | 2.5715 | |
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 B1B95/3-21G*
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 |
-51.898 |
0.000 |
0.000 |
| y |
0.000 |
-49.423 |
0.000 |
| z |
0.000 |
0.000 |
-53.505 |
|
| Traceless |
| | x | y | z |
| x |
-0.434 |
0.000 |
0.000 |
| y |
0.000 |
3.279 |
0.000 |
| z |
0.000 |
0.000 |
-2.845 |
|
| Polar |
| 3z2-r2 | -5.690 |
| x2-y2 | -2.475 |
| 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 |
3.837 |
0.000 |
0.000 |
| y |
0.000 |
11.173 |
0.000 |
| z |
0.000 |
0.000 |
16.004 |
<r2> (average value of r
2) Å
2
| <r2> |
194.888 |
| (<r2>)1/2 |
13.960 |