Jump to
S1C2
S1C3
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -1575.192478 |
| Energy at 298.15K | |
| HF Energy | -1575.192478 |
| Nuclear repulsion energy | 344.663725 |
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/STO-3G
| 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 |
642 |
565 |
0.00 |
24.84 |
0.09 |
0.16 |
| 2 |
A1 |
161 |
142 |
0.00 |
1.76 |
0.73 |
0.84 |
| 3 |
B1 |
587 |
516 |
0.00 |
15.41 |
0.75 |
0.86 |
| 4 |
B2 |
346 |
304 |
0.99 |
6.08 |
0.75 |
0.86 |
| 5 |
E |
575 |
505 |
1.61 |
3.45 |
0.75 |
0.86 |
| 5 |
E |
575 |
505 |
1.61 |
3.45 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1443.1 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 1268.4 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/STO-3G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.473 |
0.256 |
| S2 |
0.000 |
-1.473 |
0.256 |
| S3 |
-1.473 |
0.000 |
-0.256 |
| S4 |
1.473 |
0.000 |
-0.256 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9452 | 2.1446 | 2.1446 |
S2 | 2.9452 | | 2.1446 | 2.1446 | S3 | 2.1446 | 2.1446 | | 2.9452 | S4 | 2.1446 | 2.1446 | 2.9452 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
46.635 |
|
S1 |
S3 |
S4 |
46.635 |
| S2 |
S1 |
S3 |
46.635 |
|
S2 |
S4 |
S3 |
46.635 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
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 |
-43.857 |
0.000 |
0.000 |
| y |
0.000 |
-43.857 |
0.000 |
| z |
0.000 |
0.000 |
-45.793 |
|
| Traceless |
| | x | y | z |
| x |
0.968 |
0.000 |
0.000 |
| y |
0.000 |
0.968 |
0.000 |
| z |
0.000 |
0.000 |
-1.935 |
|
| Polar |
| 3z2-r2 | -3.870 |
| 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 |
5.838 |
0.000 |
0.000 |
| y |
0.000 |
5.838 |
0.000 |
| z |
0.000 |
0.000 |
0.895 |
<r2> (average value of r
2) Å
2
| <r2> |
170.777 |
| (<r2>)1/2 |
13.068 |
Jump to
S1C1
S1C3
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -1575.156402 |
| Energy at 298.15K | |
| HF Energy | -1575.156402 |
| Nuclear repulsion energy | 329.389731 |
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/STO-3G
| 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 |
766 |
673 |
0.01 |
15.32 |
0.20 |
0.33 |
| 2 |
A1 |
405 |
356 |
6.36 |
13.51 |
0.23 |
0.37 |
| 3 |
A1 |
141 |
124 |
4.06 |
3.89 |
0.51 |
0.68 |
| 4 |
A2 |
203 |
179 |
0.00 |
0.03 |
0.75 |
0.86 |
| 5 |
B2 |
771 |
678 |
30.40 |
0.65 |
0.75 |
0.86 |
| 6 |
B2 |
339 |
298 |
0.54 |
8.72 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1312.7 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 1153.7 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/STO-3G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.121 |
0.963 |
| S2 |
0.000 |
-1.121 |
0.963 |
| S3 |
0.000 |
1.462 |
-0.963 |
| S4 |
0.000 |
-1.462 |
-0.963 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.2416 | 1.9557 | 3.2218 |
S2 | 2.2416 | | 3.2218 | 1.9557 | S3 | 1.9557 | 3.2218 | | 2.9243 | S4 | 3.2218 | 1.9557 | 2.9243 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
100.052 |
|
S1 |
S3 |
S4 |
79.948 |
| S2 |
S1 |
S3 |
100.052 |
|
S2 |
S4 |
S3 |
79.948 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/STO-3G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.058 |
|
|
|
| 2 |
S |
0.058 |
|
|
|
| 3 |
S |
-0.058 |
|
|
|
| 4 |
S |
-0.058 |
|
|
|
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 |
1.121 |
1.121 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-42.421 |
0.000 |
0.000 |
| y |
0.000 |
-45.167 |
0.000 |
| z |
0.000 |
0.000 |
-44.755 |
|
| Traceless |
| | x | y | z |
| x |
2.540 |
0.000 |
0.000 |
| y |
0.000 |
-1.580 |
0.000 |
| z |
0.000 |
0.000 |
-0.961 |
|
| Polar |
| 3z2-r2 | -1.922 |
| x2-y2 | 2.747 |
| 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 |
1.211 |
0.000 |
0.000 |
| y |
0.000 |
9.448 |
0.000 |
| z |
0.000 |
0.000 |
6.311 |
<r2> (average value of r
2) Å
2
| <r2> |
195.499 |
| (<r2>)1/2 |
13.982 |
Jump to
S1C1
S1C2
Energy calculated at mPW1PW91/STO-3G
| | hartrees |
| Energy at 0K | -1575.154442 |
| Energy at 298.15K | |
| HF Energy | -1575.154442 |
| Nuclear repulsion energy | 331.753015 |
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/STO-3G
| 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 |
818 |
719 |
0.00 |
15.64 |
0.23 |
0.37 |
| 2 |
Ag |
379 |
333 |
0.00 |
16.54 |
0.26 |
0.41 |
| 3 |
Au |
231 |
203 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
801 |
704 |
37.23 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
131i |
115i |
20.47 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
347 |
305 |
0.00 |
9.08 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1222.4 cm
-1
Scaled (by 0.8789) Zero Point Vibrational Energy (zpe) 1074.4 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/STO-3G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.970 |
1.265 |
| S2 |
0.000 |
0.970 |
-1.265 |
| S3 |
0.000 |
-0.970 |
1.265 |
| S4 |
0.000 |
-0.970 |
-1.265 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5301 | 1.9397 | 3.1881 |
S2 | 2.5301 | | 3.1881 | 1.9397 | S3 | 1.9397 | 3.1881 | | 2.5301 | S4 | 3.1881 | 1.9397 | 2.5301 | |
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/STO-3G
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 |
-42.427 |
0.000 |
0.000 |
| y |
0.000 |
-44.657 |
0.000 |
| z |
0.000 |
0.000 |
-44.284 |
|
| Traceless |
| | x | y | z |
| x |
2.044 |
0.000 |
0.000 |
| y |
0.000 |
-1.301 |
0.000 |
| z |
0.000 |
0.000 |
-0.743 |
|
| Polar |
| 3z2-r2 | -1.485 |
| x2-y2 | 2.230 |
| 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 |
1.192 |
0.000 |
0.000 |
| y |
0.000 |
6.528 |
0.000 |
| z |
0.000 |
0.000 |
9.033 |
<r2> (average value of r
2) Å
2
| <r2> |
189.972 |
| (<r2>)1/2 |
13.783 |