Jump to
S1C2
S1C3
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -1592.721986 |
| Energy at 298.15K | |
| HF Energy | -1592.721986 |
| Nuclear repulsion energy | 323.897032 |
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 B1B95/6-31G
| 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 |
461 |
440 |
0.00 |
55.77 |
0.07 |
0.12 |
| 2 |
A1 |
164 |
156 |
0.00 |
7.67 |
0.75 |
0.86 |
| 3 |
B1 |
372 |
355 |
0.00 |
35.44 |
0.75 |
0.86 |
| 4 |
B2 |
273 |
261 |
0.38 |
15.13 |
0.75 |
0.86 |
| 5 |
E |
370 |
353 |
0.10 |
10.15 |
0.75 |
0.86 |
| 5 |
E |
370 |
353 |
0.10 |
10.15 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1005.1 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 958.6 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 B1B95/6-31G
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.544 |
0.353 |
| S2 |
0.000 |
-1.544 |
0.353 |
| S3 |
-1.544 |
0.000 |
-0.353 |
| S4 |
1.544 |
0.000 |
-0.353 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.0876 | 2.2947 | 2.2947 |
S2 | 3.0876 | | 2.2947 | 2.2947 | S3 | 2.2947 | 2.2947 | | 3.0876 | S4 | 2.2947 | 2.2947 | 3.0876 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.719 |
|
S1 |
S3 |
S4 |
47.719 |
| S2 |
S1 |
S3 |
47.719 |
|
S2 |
S4 |
S3 |
47.719 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
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 |
-51.439 |
0.000 |
0.000 |
| y |
0.000 |
-51.439 |
0.000 |
| z |
0.000 |
0.000 |
-55.968 |
|
| Traceless |
| | x | y | z |
| x |
2.265 |
0.000 |
0.000 |
| y |
0.000 |
2.265 |
0.000 |
| z |
0.000 |
0.000 |
-4.529 |
|
| Polar |
| 3z2-r2 | -9.059 |
| 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 |
12.311 |
0.000 |
0.000 |
| y |
0.000 |
12.311 |
0.000 |
| z |
0.000 |
0.000 |
4.721 |
<r2> (average value of r
2) Å
2
| <r2> |
193.584 |
| (<r2>)1/2 |
13.913 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -1592.736640 |
| Energy at 298.15K | |
| HF Energy | -1592.736640 |
| Nuclear repulsion energy | 313.180424 |
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 B1B95/6-31G
| 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 |
616 |
587 |
0.01 |
38.59 |
0.27 |
0.42 |
| 2 |
A1 |
283 |
270 |
1.78 |
33.23 |
0.27 |
0.42 |
| 3 |
A1 |
56 |
53 |
8.25 |
1.97 |
0.57 |
0.73 |
| 4 |
A2 |
195 |
186 |
0.00 |
0.02 |
0.75 |
0.86 |
| 5 |
B2 |
588 |
561 |
95.25 |
0.42 |
0.75 |
0.86 |
| 6 |
B2 |
271 |
258 |
0.03 |
21.03 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1003.9 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 957.4 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 B1B95/6-31G
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.249 |
1.014 |
| S2 |
0.000 |
-1.249 |
1.014 |
| S3 |
0.000 |
1.468 |
-1.014 |
| S4 |
0.000 |
-1.468 |
-1.014 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4970 | 2.0393 | 3.3897 |
S2 | 2.4970 | | 3.3897 | 2.0393 | S3 | 2.0393 | 3.3897 | | 2.9361 | S4 | 3.3897 | 2.0393 | 2.9361 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
96.180 |
|
S1 |
S3 |
S4 |
83.820 |
| S2 |
S1 |
S3 |
96.180 |
|
S2 |
S4 |
S3 |
83.820 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.022 |
|
|
|
| 2 |
S |
0.022 |
|
|
|
| 3 |
S |
-0.022 |
|
|
|
| 4 |
S |
-0.022 |
|
|
|
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 |
0.621 |
0.621 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.574 |
0.000 |
0.000 |
| y |
0.000 |
-54.988 |
0.000 |
| z |
0.000 |
0.000 |
-51.940 |
|
| Traceless |
| | x | y | z |
| x |
0.890 |
0.000 |
0.000 |
| y |
0.000 |
-2.731 |
0.000 |
| z |
0.000 |
0.000 |
1.841 |
|
| Polar |
| 3z2-r2 | 3.683 |
| x2-y2 | 2.414 |
| 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 |
3.325 |
0.000 |
0.000 |
| y |
0.000 |
17.905 |
0.000 |
| z |
0.000 |
0.000 |
12.978 |
<r2> (average value of r
2) Å
2
| <r2> |
217.824 |
| (<r2>)1/2 |
14.759 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/6-31G
| | hartrees |
| Energy at 0K | -1592.736611 |
| Energy at 298.15K | |
| HF Energy | -1592.736611 |
| Nuclear repulsion energy | 313.984438 |
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 B1B95/6-31G
| 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 |
627 |
598 |
0.00 |
39.63 |
0.28 |
0.44 |
| 2 |
Ag |
282 |
269 |
0.00 |
33.69 |
0.28 |
0.43 |
| 3 |
Au |
201 |
192 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
593 |
565 |
98.97 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
29 |
28 |
11.71 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
270 |
258 |
0.00 |
21.35 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1001.1 cm
-1
Scaled (by 0.9537) Zero Point Vibrational Energy (zpe) 954.7 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 B1B95/6-31G
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.017 |
1.347 |
| S2 |
0.000 |
1.017 |
-1.347 |
| S3 |
0.000 |
-1.017 |
1.347 |
| S4 |
0.000 |
-1.017 |
-1.347 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6939 | 2.0348 | 3.3760 |
S2 | 2.6939 | | 3.3760 | 2.0348 | S3 | 2.0348 | 3.3760 | | 2.6939 | S4 | 3.3760 | 2.0348 | 2.6939 | |
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 B1B95/6-31G
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 |
-52.619 |
0.000 |
0.000 |
| y |
0.000 |
-51.880 |
0.000 |
| z |
0.000 |
0.000 |
-54.878 |
|
| Traceless |
| | x | y | z |
| x |
0.760 |
0.000 |
0.000 |
| y |
0.000 |
1.868 |
0.000 |
| z |
0.000 |
0.000 |
-2.628 |
|
| Polar |
| 3z2-r2 | -5.257 |
| x2-y2 | -0.739 |
| 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 |
3.322 |
0.000 |
0.000 |
| y |
0.000 |
13.081 |
0.000 |
| z |
0.000 |
0.000 |
17.680 |
<r2> (average value of r
2) Å
2
| <r2> |
215.538 |
| (<r2>)1/2 |
14.681 |