Jump to
S1C2
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -1582.600872 |
| Energy at 298.15K | |
| HF Energy | -1582.600872 |
| Nuclear repulsion energy | 351.211480 |
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 HF/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 |
535 |
483 |
0.00 |
77.39 |
0.08 |
0.15 |
| 2 |
A1 |
191 |
172 |
0.00 |
2.81 |
0.74 |
0.85 |
| 3 |
B1 |
505 |
456 |
0.00 |
43.50 |
0.75 |
0.86 |
| 4 |
B2 |
374 |
337 |
0.88 |
10.75 |
0.75 |
0.86 |
| 5 |
E |
476 |
430 |
0.10 |
9.96 |
0.75 |
0.86 |
| 5 |
E |
476 |
430 |
0.10 |
9.96 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1278.2 cm
-1
Scaled (by 0.9026) 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 HF/3-21G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.437 |
0.281 |
| S2 |
0.000 |
-1.437 |
0.281 |
| S3 |
-1.437 |
0.000 |
-0.281 |
| S4 |
1.437 |
0.000 |
-0.281 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8743 | 2.1089 | 2.1089 |
S2 | 2.8743 | | 2.1089 | 2.1089 | S3 | 2.1089 | 2.1089 | | 2.8743 | S4 | 2.1089 | 2.1089 | 2.8743 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.040 |
|
S1 |
S3 |
S4 |
47.040 |
| S2 |
S1 |
S3 |
47.040 |
|
S2 |
S4 |
S3 |
47.040 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/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 |
-51.291 |
0.000 |
0.000 |
| y |
0.000 |
-51.291 |
0.000 |
| z |
0.000 |
0.000 |
-56.556 |
|
| Traceless |
| | x | y | z |
| x |
2.633 |
0.000 |
0.000 |
| y |
0.000 |
2.633 |
0.000 |
| z |
0.000 |
0.000 |
-5.265 |
|
| Polar |
| 3z2-r2 | -10.531 |
| 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 |
10.111 |
0.000 |
0.000 |
| y |
0.000 |
10.111 |
0.000 |
| z |
0.000 |
0.000 |
4.513 |
<r2> (average value of r
2) Å
2
| <r2> |
170.384 |
| (<r2>)1/2 |
13.053 |
Jump to
S1C1
S1C3
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -1582.585756 |
| Energy at 298.15K | |
| HF Energy | -1582.585756 |
| Nuclear repulsion energy | 335.671724 |
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 HF/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 |
646 |
7.00 |
26.07 |
0.47 |
0.64 |
| 2 |
A1 |
551 |
497 |
5.35 |
323.53 |
0.26 |
0.41 |
| 3 |
A1 |
146 |
132 |
0.01 |
27.51 |
0.46 |
0.63 |
| 4 |
A2 |
224 |
202 |
0.00 |
0.78 |
0.75 |
0.86 |
| 5 |
B2 |
640 |
577 |
449.03 |
0.01 |
0.75 |
0.86 |
| 6 |
B2 |
377 |
340 |
1.61 |
12.66 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1326.8 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 1197.6 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 HF/3-21G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.990 |
0.888 |
| S2 |
0.000 |
-0.990 |
0.888 |
| S3 |
0.000 |
1.677 |
-0.888 |
| S4 |
0.000 |
-1.677 |
-0.888 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 1.9797 | 1.9040 | 3.2041 |
S2 | 1.9797 | | 3.2041 | 1.9040 | S3 | 1.9040 | 3.2041 | | 3.3544 | S4 | 3.2041 | 1.9040 | 3.3544 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
111.161 |
|
S1 |
S3 |
S4 |
68.839 |
| S2 |
S1 |
S3 |
111.161 |
|
S2 |
S4 |
S3 |
68.839 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.165 |
|
|
|
| 2 |
S |
0.165 |
|
|
|
| 3 |
S |
-0.165 |
|
|
|
| 4 |
S |
-0.165 |
|
|
|
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 |
2.381 |
2.381 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.507 |
0.000 |
0.000 |
| y |
0.000 |
-56.612 |
0.000 |
| z |
0.000 |
0.000 |
-51.834 |
|
| Traceless |
| | x | y | z |
| x |
1.715 |
0.000 |
0.000 |
| y |
0.000 |
-4.442 |
0.000 |
| z |
0.000 |
0.000 |
2.726 |
|
| Polar |
| 3z2-r2 | 5.452 |
| x2-y2 | 4.105 |
| 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 |
3.857 |
0.000 |
0.000 |
| y |
0.000 |
22.013 |
0.000 |
| z |
0.000 |
0.000 |
10.068 |
<r2> (average value of r
2) Å
2
| <r2> |
205.326 |
| (<r2>)1/2 |
14.329 |
Jump to
S1C1
S1C2
Energy calculated at HF/3-21G*
| | hartrees |
| Energy at 0K | -1582.559285 |
| Energy at 298.15K | |
| HF Energy | -1582.559285 |
| Nuclear repulsion energy | 338.100814 |
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 HF/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 |
830 |
750 |
0.00 |
43.83 |
0.43 |
0.60 |
| 2 |
Ag |
331 |
298 |
0.00 |
6946.43 |
0.33 |
0.50 |
| 3 |
Au |
279 |
252 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
692 |
624 |
908.04 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
253i |
229i |
42.85 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
380 |
343 |
0.00 |
11.74 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1129.3 cm
-1
Scaled (by 0.9026) Zero Point Vibrational Energy (zpe) 1019.3 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 HF/3-21G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.931 |
1.271 |
| S2 |
0.000 |
0.931 |
-1.271 |
| S3 |
0.000 |
-0.931 |
1.271 |
| S4 |
0.000 |
-0.931 |
-1.271 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5430 | 1.8611 | 3.1513 |
S2 | 2.5430 | | 3.1513 | 1.8611 | S3 | 1.8611 | 3.1513 | | 2.5430 | S4 | 3.1513 | 1.8611 | 2.5430 | |
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 HF/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 |
-53.146 |
0.000 |
0.000 |
| y |
0.000 |
-50.907 |
0.000 |
| z |
0.000 |
0.000 |
-55.222 |
|
| Traceless |
| | x | y | z |
| x |
-0.081 |
0.000 |
0.000 |
| y |
0.000 |
3.277 |
0.000 |
| z |
0.000 |
0.000 |
-3.196 |
|
| Polar |
| 3z2-r2 | -6.392 |
| x2-y2 | -2.239 |
| 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 |
3.760 |
0.000 |
0.000 |
| y |
0.000 |
11.095 |
0.000 |
| z |
0.000 |
0.000 |
25.392 |
<r2> (average value of r
2) Å
2
| <r2> |
192.047 |
| (<r2>)1/2 |
13.858 |