Jump to
S1C2
S1C3
Energy calculated at mPW1PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.862628 |
| Energy at 298.15K | |
| HF Energy | -1584.862628 |
| Nuclear repulsion energy | 318.521672 |
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 mPW1PW91/3-21G
| 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 |
462 |
441 |
0.00 |
48.03 |
0.06 |
0.11 |
| 2 |
A1 |
154 |
147 |
0.00 |
9.82 |
0.75 |
0.86 |
| 3 |
B1 |
371 |
354 |
0.00 |
30.59 |
0.75 |
0.86 |
| 4 |
B2 |
266 |
254 |
0.26 |
16.83 |
0.75 |
0.86 |
| 5 |
E |
367 |
350 |
0.01 |
9.75 |
0.75 |
0.86 |
| 5 |
E |
367 |
350 |
0.01 |
9.75 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 993.3 cm
-1
Scaled (by 0.9546) Zero Point Vibrational Energy (zpe) 948.2 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 mPW1PW91/3-21G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.568 |
0.364 |
| S2 |
0.000 |
-1.568 |
0.364 |
| S3 |
-1.568 |
0.000 |
-0.364 |
| S4 |
1.568 |
0.000 |
-0.364 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.1363 | 2.3343 | 2.3343 |
S2 | 3.1363 | | 2.3343 | 2.3343 | S3 | 2.3343 | 2.3343 | | 3.1363 | S4 | 2.3343 | 2.3343 | 3.1363 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.795 |
|
S1 |
S3 |
S4 |
47.795 |
| S2 |
S1 |
S3 |
47.795 |
|
S2 |
S4 |
S3 |
47.795 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G
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 |
-51.989 |
0.000 |
0.000 |
| y |
0.000 |
-51.989 |
0.000 |
| z |
0.000 |
0.000 |
-56.797 |
|
| Traceless |
| | x | y | z |
| x |
2.404 |
0.000 |
0.000 |
| y |
0.000 |
2.404 |
0.000 |
| z |
0.000 |
0.000 |
-4.808 |
|
| Polar |
| 3z2-r2 | -9.616 |
| 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 |
12.386 |
0.000 |
0.000 |
| y |
0.000 |
12.386 |
0.000 |
| z |
0.000 |
0.000 |
4.223 |
<r2> (average value of r
2) Å
2
| <r2> |
199.351 |
| (<r2>)1/2 |
14.119 |
Jump to
S1C1
S1C3
Energy calculated at mPW1PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.874049 |
| Energy at 298.15K | |
| HF Energy | -1584.874049 |
| Nuclear repulsion energy | 312.161337 |
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 mPW1PW91/3-21G
| 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 |
585 |
559 |
0.00 |
33.88 |
0.28 |
0.44 |
| 2 |
A1 |
307 |
293 |
0.00 |
32.61 |
0.27 |
0.42 |
| 3 |
A1 |
103 |
98 |
8.88 |
0.00 |
0.52 |
0.69 |
| 4 |
A2 |
203 |
194 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
549 |
524 |
81.56 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
279 |
267 |
0.00 |
21.73 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1012.9 cm
-1
Scaled (by 0.9546) Zero Point Vibrational Energy (zpe) 966.9 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 mPW1PW91/3-21G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.345 |
1.030 |
| S2 |
0.000 |
-1.345 |
1.030 |
| S3 |
0.000 |
1.345 |
-1.030 |
| S4 |
0.000 |
-1.345 |
-1.030 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6896 | 2.0609 | 3.3884 |
S2 | 2.6896 | | 3.3884 | 2.0609 | S3 | 2.0609 | 3.3884 | | 2.6898 | S4 | 3.3884 | 2.0609 | 2.6898 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.002 |
|
S1 |
S3 |
S4 |
89.998 |
| S2 |
S1 |
S3 |
90.002 |
|
S2 |
S4 |
S3 |
89.998 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/3-21G
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 |
-53.451 |
0.000 |
0.000 |
| y |
0.000 |
-55.545 |
0.000 |
| z |
0.000 |
0.000 |
-52.285 |
|
| Traceless |
| | x | y | z |
| x |
0.464 |
0.000 |
0.000 |
| y |
0.000 |
-2.677 |
0.000 |
| z |
0.000 |
0.000 |
2.213 |
|
| Polar |
| 3z2-r2 | 4.427 |
| x2-y2 | 2.094 |
| 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 |
2.798 |
0.000 |
0.000 |
| y |
0.000 |
16.822 |
0.000 |
| z |
0.000 |
0.000 |
13.038 |
<r2> (average value of r
2) Å
2
| <r2> |
217.282 |
| (<r2>)1/2 |
14.740 |
Jump to
S1C1
S1C2
Energy calculated at mPW1PW91/3-21G
| | hartrees |
| Energy at 0K | -1584.874049 |
| Energy at 298.15K | |
| HF Energy | -1584.874049 |
| Nuclear repulsion energy | 312.167882 |
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 mPW1PW91/3-21G
| 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 |
585 |
559 |
0.00 |
33.88 |
0.28 |
0.44 |
| 2 |
Ag |
307 |
293 |
0.00 |
32.61 |
0.27 |
0.42 |
| 3 |
Au |
203 |
194 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
549 |
524 |
81.56 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
103 |
98 |
8.88 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
279 |
267 |
0.00 |
21.73 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1013.0 cm
-1
Scaled (by 0.9546) Zero Point Vibrational Energy (zpe) 967.0 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 mPW1PW91/3-21G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.030 |
1.345 |
| S2 |
0.000 |
1.030 |
-1.345 |
| S3 |
0.000 |
-1.030 |
1.345 |
| S4 |
0.000 |
-1.030 |
-1.345 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6896 | 2.0608 | 3.3884 |
S2 | 2.6896 | | 3.3884 | 2.0608 | S3 | 2.0608 | 3.3884 | | 2.6896 | S4 | 3.3884 | 2.0608 | 2.6896 | |
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 mPW1PW91/3-21G
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 |
-53.451 |
0.000 |
0.000 |
| y |
0.000 |
-52.285 |
0.000 |
| z |
0.000 |
0.000 |
-55.546 |
|
| Traceless |
| | x | y | z |
| x |
0.464 |
0.000 |
0.000 |
| y |
0.000 |
2.214 |
0.000 |
| z |
0.000 |
0.000 |
-2.678 |
|
| Polar |
| 3z2-r2 | -5.355 |
| x2-y2 | -1.166 |
| 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 |
2.798 |
0.000 |
0.000 |
| y |
0.000 |
13.038 |
0.000 |
| z |
0.000 |
0.000 |
16.821 |
<r2> (average value of r
2) Å
2
| <r2> |
217.273 |
| (<r2>)1/2 |
14.740 |