Jump to
S1C2
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -1592.935520 |
| Energy at 298.15K | |
| HF Energy | -1592.935520 |
| Nuclear repulsion energy | 349.461478 |
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 B1B95/6-311G*
| 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 |
517 |
496 |
0.00 |
51.86 |
0.07 |
0.14 |
| 2 |
A1 |
204 |
196 |
0.00 |
3.47 |
0.69 |
0.82 |
| 3 |
B1 |
443 |
424 |
0.00 |
36.85 |
0.75 |
0.86 |
| 4 |
B2 |
304 |
292 |
0.09 |
9.61 |
0.75 |
0.86 |
| 5 |
E |
430 |
412 |
0.10 |
7.95 |
0.75 |
0.86 |
| 5 |
E |
430 |
412 |
0.10 |
7.95 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1163.6 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 1115.4 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 B1B95/6-311G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.430 |
0.331 |
| S2 |
0.000 |
-1.430 |
0.331 |
| S3 |
-1.430 |
0.000 |
-0.331 |
| S4 |
1.430 |
0.000 |
-0.331 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8596 | 2.1274 | 2.1274 |
S2 | 2.8596 | | 2.1274 | 2.1274 | S3 | 2.1274 | 2.1274 | | 2.8596 | S4 | 2.1274 | 2.1274 | 2.8596 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.771 |
|
S1 |
S3 |
S4 |
47.771 |
| S2 |
S1 |
S3 |
47.771 |
|
S2 |
S4 |
S3 |
47.771 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
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 |
-50.238 |
0.000 |
0.000 |
| y |
0.000 |
-50.238 |
0.000 |
| z |
0.000 |
0.000 |
-55.293 |
|
| Traceless |
| | x | y | z |
| x |
2.528 |
0.000 |
0.000 |
| y |
0.000 |
2.528 |
0.000 |
| z |
0.000 |
0.000 |
-5.056 |
|
| Polar |
| 3z2-r2 | -10.111 |
| 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 |
10.590 |
0.000 |
0.000 |
| y |
0.000 |
10.590 |
0.000 |
| z |
0.000 |
0.000 |
5.657 |
<r2> (average value of r
2) Å
2
| <r2> |
170.262 |
| (<r2>)1/2 |
13.048 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -1592.959473 |
| Energy at 298.15K | |
| HF Energy | -1592.959473 |
| Nuclear repulsion energy | 331.655231 |
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 B1B95/6-311G*
| 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 |
682 |
654 |
3.11 |
33.39 |
0.23 |
0.37 |
| 2 |
A1 |
341 |
327 |
8.54 |
39.68 |
0.24 |
0.39 |
| 3 |
A1 |
88 |
85 |
1.86 |
9.01 |
0.48 |
0.64 |
| 4 |
A2 |
218 |
209 |
0.00 |
0.19 |
0.75 |
0.86 |
| 5 |
B2 |
653 |
626 |
160.03 |
3.83 |
0.75 |
0.86 |
| 6 |
B2 |
333 |
319 |
0.01 |
13.61 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1157.6 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 1109.7 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 B1B95/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.079 |
0.923 |
| S2 |
0.000 |
-1.079 |
0.923 |
| S3 |
0.000 |
1.570 |
-0.923 |
| S4 |
0.000 |
-1.570 |
-0.923 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1576 | 1.9106 | 3.2287 |
S2 | 2.1576 | | 3.2287 | 1.9106 | S3 | 1.9106 | 3.2287 | | 3.1397 | S4 | 3.2287 | 1.9106 | 3.1397 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
104.893 |
|
S1 |
S3 |
S4 |
75.107 |
| S2 |
S1 |
S3 |
104.893 |
|
S2 |
S4 |
S3 |
75.107 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.120 |
|
|
|
| 2 |
S |
0.120 |
|
|
|
| 3 |
S |
-0.120 |
|
|
|
| 4 |
S |
-0.120 |
|
|
|
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 |
1.671 |
1.671 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.101 |
0.000 |
0.000 |
| y |
0.000 |
-55.160 |
0.000 |
| z |
0.000 |
0.000 |
-50.268 |
|
| Traceless |
| | x | y | z |
| x |
0.613 |
0.000 |
0.000 |
| y |
0.000 |
-3.975 |
0.000 |
| z |
0.000 |
0.000 |
3.362 |
|
| Polar |
| 3z2-r2 | 6.725 |
| x2-y2 | 3.059 |
| 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 |
4.503 |
0.000 |
0.000 |
| y |
0.000 |
18.908 |
0.000 |
| z |
0.000 |
0.000 |
11.618 |
<r2> (average value of r
2) Å
2
| <r2> |
203.452 |
| (<r2>)1/2 |
14.264 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-311G*
| | hartrees |
| Energy at 0K | -1592.957010 |
| Energy at 298.15K | |
| HF Energy | -1592.957010 |
| Nuclear repulsion energy | 334.767887 |
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 B1B95/6-311G*
| 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 |
735 |
704 |
0.00 |
40.95 |
0.27 |
0.42 |
| 2 |
Ag |
295 |
282 |
0.00 |
37.22 |
0.29 |
0.45 |
| 3 |
Au |
249 |
239 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
684 |
655 |
168.76 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
95i |
92i |
25.67 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
333 |
319 |
0.00 |
15.01 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1099.6 cm
-1
Scaled (by 0.9586) Zero Point Vibrational Energy (zpe) 1054.1 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 B1B95/6-311G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.947 |
1.274 |
| S2 |
0.000 |
0.947 |
-1.274 |
| S3 |
0.000 |
-0.947 |
1.274 |
| S4 |
0.000 |
-0.947 |
-1.274 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5485 | 1.8932 | 3.1747 |
S2 | 2.5485 | | 3.1747 | 1.8932 | S3 | 1.8932 | 3.1747 | | 2.5485 | S4 | 3.1747 | 1.8932 | 2.5485 | |
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 B1B95/6-311G*
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 |
-52.423 |
0.000 |
0.000 |
| y |
0.000 |
-49.671 |
0.000 |
| z |
0.000 |
0.000 |
-54.534 |
|
| Traceless |
| | x | y | z |
| x |
-0.321 |
0.000 |
0.000 |
| y |
0.000 |
3.807 |
0.000 |
| z |
0.000 |
0.000 |
-3.487 |
|
| Polar |
| 3z2-r2 | -6.974 |
| x2-y2 | -2.752 |
| 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 |
4.484 |
0.000 |
0.000 |
| y |
0.000 |
12.085 |
0.000 |
| z |
0.000 |
0.000 |
18.121 |
<r2> (average value of r
2) Å
2
| <r2> |
193.872 |
| (<r2>)1/2 |
13.924 |