Jump to
S1C2
S1C3
Energy calculated at mPW1PW91/6-31+G**
| | hartrees |
| Energy at 0K | -1592.718070 |
| Energy at 298.15K | |
| HF Energy | -1592.718070 |
| Nuclear repulsion energy | 348.571214 |
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 mPW1PW91/6-31+G**
| 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 |
515 |
491 |
0.00 |
49.21 |
0.07 |
0.13 |
| 2 |
A1 |
201 |
191 |
0.00 |
0.90 |
0.63 |
0.77 |
| 3 |
B1 |
451 |
429 |
0.00 |
38.18 |
0.75 |
0.86 |
| 4 |
B2 |
313 |
298 |
0.17 |
8.53 |
0.75 |
0.86 |
| 5 |
E |
431 |
410 |
0.05 |
5.80 |
0.75 |
0.86 |
| 5 |
E |
431 |
410 |
0.05 |
5.80 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1170.6 cm
-1
Scaled (by 0.9518) Zero Point Vibrational Energy (zpe) 1114.2 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 mPW1PW91/6-31+G**
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.439 |
0.313 |
| S2 |
0.000 |
-1.439 |
0.313 |
| S3 |
-1.439 |
0.000 |
-0.313 |
| S4 |
1.439 |
0.000 |
-0.313 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8785 | 2.1296 | 2.1296 |
S2 | 2.8785 | | 2.1296 | 2.1296 | S3 | 2.1296 | 2.1296 | | 2.8785 | S4 | 2.1296 | 2.1296 | 2.8785 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.482 |
|
S1 |
S3 |
S4 |
47.482 |
| S2 |
S1 |
S3 |
47.482 |
|
S2 |
S4 |
S3 |
47.482 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31+G**
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 |
-49.839 |
0.000 |
0.000 |
| y |
0.000 |
-49.839 |
0.000 |
| z |
0.000 |
0.000 |
-55.331 |
|
| Traceless |
| | x | y | z |
| x |
2.746 |
0.000 |
0.000 |
| y |
0.000 |
2.746 |
0.000 |
| z |
0.000 |
0.000 |
-5.492 |
|
| Polar |
| 3z2-r2 | -10.984 |
| 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 |
11.106 |
0.000 |
0.000 |
| y |
0.000 |
11.106 |
0.000 |
| z |
0.000 |
0.000 |
7.518 |
<r2> (average value of r
2) Å
2
| <r2> |
171.123 |
| (<r2>)1/2 |
13.081 |
Jump to
S1C1
S1C3
Energy calculated at mPW1PW91/6-31+G**
| | hartrees |
| Energy at 0K | -1592.745005 |
| Energy at 298.15K | |
| HF Energy | -1592.745005 |
| Nuclear repulsion energy | 330.324925 |
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 mPW1PW91/6-31+G**
| 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 |
688 |
655 |
3.33 |
33.16 |
0.13 |
0.23 |
| 2 |
A1 |
361 |
343 |
7.45 |
34.71 |
0.19 |
0.32 |
| 3 |
A1 |
106 |
101 |
0.99 |
10.31 |
0.50 |
0.67 |
| 4 |
A2 |
214 |
204 |
0.00 |
0.88 |
0.75 |
0.86 |
| 5 |
B2 |
663 |
631 |
142.16 |
3.82 |
0.75 |
0.86 |
| 6 |
B2 |
335 |
319 |
0.05 |
12.12 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1183.4 cm
-1
Scaled (by 0.9518) Zero Point Vibrational Energy (zpe) 1126.3 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 mPW1PW91/6-31+G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.071 |
0.922 |
| S2 |
0.000 |
-1.071 |
0.922 |
| S3 |
0.000 |
1.598 |
-0.922 |
| S4 |
0.000 |
-1.598 |
-0.922 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1423 | 1.9186 | 3.2449 |
S2 | 2.1423 | | 3.2449 | 1.9186 | S3 | 1.9186 | 3.2449 | | 3.1969 | S4 | 3.2449 | 1.9186 | 3.1969 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
105.953 |
|
S1 |
S3 |
S4 |
74.047 |
| S2 |
S1 |
S3 |
105.953 |
|
S2 |
S4 |
S3 |
74.047 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.119 |
|
|
|
| 2 |
S |
0.119 |
|
|
|
| 3 |
S |
-0.119 |
|
|
|
| 4 |
S |
-0.119 |
|
|
|
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 |
1.603 |
1.603 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.673 |
0.000 |
0.000 |
| y |
0.000 |
-54.415 |
0.000 |
| z |
0.000 |
0.000 |
-50.113 |
|
| Traceless |
| | x | y | z |
| x |
0.592 |
0.000 |
0.000 |
| y |
0.000 |
-3.523 |
0.000 |
| z |
0.000 |
0.000 |
2.931 |
|
| Polar |
| 3z2-r2 | 5.862 |
| x2-y2 | 2.743 |
| 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 |
6.141 |
0.000 |
0.000 |
| y |
0.000 |
19.183 |
0.000 |
| z |
0.000 |
0.000 |
11.875 |
<r2> (average value of r
2) Å
2
| <r2> |
205.444 |
| (<r2>)1/2 |
14.333 |
Jump to
S1C1
S1C2
Energy calculated at mPW1PW91/6-31+G**
| | hartrees |
| Energy at 0K | -1592.741478 |
| Energy at 298.15K | |
| HF Energy | -1592.741478 |
| Nuclear repulsion energy | 333.439615 |
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 mPW1PW91/6-31+G**
| 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 |
739 |
703 |
0.00 |
41.63 |
0.17 |
0.29 |
| 2 |
Ag |
292 |
278 |
0.00 |
32.58 |
0.25 |
0.41 |
| 3 |
Au |
247 |
235 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
689 |
655 |
152.75 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
111i |
106i |
21.33 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
337 |
320 |
0.00 |
13.82 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1095.8 cm
-1
Scaled (by 0.9518) Zero Point Vibrational Energy (zpe) 1042.9 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 mPW1PW91/6-31+G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.951 |
1.279 |
| S2 |
0.000 |
0.951 |
-1.279 |
| S3 |
0.000 |
-0.951 |
1.279 |
| S4 |
0.000 |
-0.951 |
-1.279 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5573 | 1.9017 | 3.1869 |
S2 | 2.5573 | | 3.1869 | 1.9017 | S3 | 1.9017 | 3.1869 | | 2.5573 | S4 | 3.1869 | 1.9017 | 2.5573 | |
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 mPW1PW91/6-31+G**
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 |
-51.998 |
0.000 |
0.000 |
| y |
0.000 |
-49.427 |
0.000 |
| z |
0.000 |
0.000 |
-54.066 |
|
| Traceless |
| | x | y | z |
| x |
-0.251 |
0.000 |
0.000 |
| y |
0.000 |
3.604 |
0.000 |
| z |
0.000 |
0.000 |
-3.353 |
|
| Polar |
| 3z2-r2 | -6.706 |
| x2-y2 | -2.570 |
| 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 |
6.373 |
0.000 |
0.000 |
| y |
0.000 |
12.280 |
0.000 |
| z |
0.000 |
0.000 |
18.170 |
<r2> (average value of r
2) Å
2
| <r2> |
194.869 |
| (<r2>)1/2 |
13.960 |