Jump to
S1C2
S1C3
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1592.804748 |
| Energy at 298.15K | |
| HF Energy | -1592.804748 |
| Nuclear repulsion energy | 342.556068 |
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 B3LYP/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 |
481 |
464 |
0.00 |
57.36 |
0.08 |
0.15 |
| 2 |
A1 |
189 |
182 |
0.00 |
3.88 |
0.71 |
0.83 |
| 3 |
B1 |
408 |
394 |
0.00 |
40.40 |
0.75 |
0.86 |
| 4 |
B2 |
299 |
289 |
0.03 |
10.57 |
0.75 |
0.86 |
| 5 |
E |
392 |
379 |
0.22 |
7.88 |
0.75 |
0.86 |
| 5 |
E |
392 |
379 |
0.22 |
7.88 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1080.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 1043.7 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 B3LYP/6-311G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.464 |
0.320 |
| S2 |
0.000 |
-1.464 |
0.320 |
| S3 |
-1.464 |
0.000 |
-0.320 |
| S4 |
1.464 |
0.000 |
-0.320 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9285 | 2.1672 | 2.1672 |
S2 | 2.9285 | | 2.1672 | 2.1672 | S3 | 2.1672 | 2.1672 | | 2.9285 | S4 | 2.1672 | 2.1672 | 2.9285 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.497 |
|
S1 |
S3 |
S4 |
47.497 |
| S2 |
S1 |
S3 |
47.497 |
|
S2 |
S4 |
S3 |
47.497 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/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 |
-50.738 |
0.000 |
0.000 |
| y |
0.000 |
-50.738 |
0.000 |
| z |
0.000 |
0.000 |
-56.109 |
|
| Traceless |
| | x | y | z |
| x |
2.686 |
0.000 |
0.000 |
| y |
0.000 |
2.686 |
0.000 |
| z |
0.000 |
0.000 |
-5.371 |
|
| Polar |
| 3z2-r2 | -10.742 |
| 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 |
11.228 |
0.000 |
0.000 |
| y |
0.000 |
11.228 |
0.000 |
| z |
0.000 |
0.000 |
5.693 |
<r2> (average value of r
2) Å
2
| <r2> |
176.563 |
| (<r2>)1/2 |
13.288 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1592.835603 |
| Energy at 298.15K | |
| HF Energy | -1592.835603 |
| Nuclear repulsion energy | 325.382391 |
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 B3LYP/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 |
649 |
627 |
2.22 |
35.25 |
0.24 |
0.39 |
| 2 |
A1 |
300 |
290 |
7.79 |
37.43 |
0.25 |
0.39 |
| 3 |
A1 |
85 |
82 |
2.06 |
8.05 |
0.49 |
0.66 |
| 4 |
A2 |
207 |
200 |
0.00 |
0.13 |
0.75 |
0.86 |
| 5 |
B2 |
622 |
601 |
150.02 |
3.47 |
0.75 |
0.86 |
| 6 |
B2 |
320 |
309 |
0.01 |
14.91 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1090.9 cm
-1
Scaled (by 0.9663) 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 B3LYP/6-311G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.114 |
0.935 |
| S2 |
0.000 |
-1.114 |
0.935 |
| S3 |
0.000 |
1.603 |
-0.935 |
| S4 |
0.000 |
-1.603 |
-0.935 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.2272 | 1.9334 | 3.2979 |
S2 | 2.2272 | | 3.2979 | 1.9334 | S3 | 1.9334 | 3.2979 | | 3.2051 | S4 | 3.2979 | 1.9334 | 3.2051 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
104.649 |
|
S1 |
S3 |
S4 |
75.351 |
| S2 |
S1 |
S3 |
104.649 |
|
S2 |
S4 |
S3 |
75.351 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.108 |
|
|
|
| 2 |
S |
0.108 |
|
|
|
| 3 |
S |
-0.108 |
|
|
|
| 4 |
S |
-0.108 |
|
|
|
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 |
1.551 |
1.551 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-52.784 |
0.000 |
0.000 |
| y |
0.000 |
-55.675 |
0.000 |
| z |
0.000 |
0.000 |
-50.760 |
|
| Traceless |
| | x | y | z |
| x |
0.433 |
0.000 |
0.000 |
| y |
0.000 |
-3.903 |
0.000 |
| z |
0.000 |
0.000 |
3.470 |
|
| Polar |
| 3z2-r2 | 6.939 |
| x2-y2 | 2.891 |
| 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 |
4.559 |
0.000 |
0.000 |
| y |
0.000 |
19.641 |
0.000 |
| z |
0.000 |
0.000 |
12.090 |
<r2> (average value of r
2) Å
2
| <r2> |
210.996 |
| (<r2>)1/2 |
14.526 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/6-311G*
| | hartrees |
| Energy at 0K | -1592.833977 |
| Energy at 298.15K | |
| HF Energy | -1592.833977 |
| Nuclear repulsion energy | 328.343237 |
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 B3LYP/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 |
692 |
669 |
0.00 |
42.23 |
0.27 |
0.43 |
| 2 |
Ag |
271 |
262 |
0.00 |
35.74 |
0.29 |
0.45 |
| 3 |
Au |
234 |
226 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
644 |
623 |
156.82 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
82i |
79i |
21.54 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
321 |
310 |
0.00 |
16.09 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1040.1 cm
-1
Scaled (by 0.9663) Zero Point Vibrational Energy (zpe) 1005.1 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 B3LYP/6-311G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.959 |
1.308 |
| S2 |
0.000 |
0.959 |
-1.308 |
| S3 |
0.000 |
-0.959 |
1.308 |
| S4 |
0.000 |
-0.959 |
-1.308 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6157 | 1.9183 | 3.2438 |
S2 | 2.6157 | | 3.2438 | 1.9183 | S3 | 1.9183 | 3.2438 | | 2.6157 | S4 | 3.2438 | 1.9183 | 2.6157 | |
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 B3LYP/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 |
-53.071 |
0.000 |
0.000 |
| y |
0.000 |
-50.158 |
0.000 |
| z |
0.000 |
0.000 |
-55.118 |
|
| Traceless |
| | x | y | z |
| x |
-0.434 |
0.000 |
0.000 |
| y |
0.000 |
3.937 |
0.000 |
| z |
0.000 |
0.000 |
-3.503 |
|
| Polar |
| 3z2-r2 | -7.006 |
| x2-y2 | -2.914 |
| 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 |
4.529 |
0.000 |
0.000 |
| y |
0.000 |
12.538 |
0.000 |
| z |
0.000 |
0.000 |
18.823 |
<r2> (average value of r
2) Å
2
| <r2> |
201.319 |
| (<r2>)1/2 |
14.189 |