Jump to
S1C2
S1C3
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -1592.557063 |
| Energy at 298.15K | |
| HF Energy | -1592.557063 |
| Nuclear repulsion energy | 348.738555 |
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 M06-2X/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 |
520 |
495 |
0.00 |
57.70 |
0.07 |
0.13 |
| 2 |
A1 |
196 |
187 |
0.00 |
2.74 |
0.74 |
0.85 |
| 3 |
B1 |
468 |
444 |
0.00 |
37.72 |
0.75 |
0.86 |
| 4 |
B2 |
325 |
309 |
0.36 |
10.70 |
0.75 |
0.86 |
| 5 |
E |
445 |
423 |
0.00 |
8.21 |
0.75 |
0.86 |
| 5 |
E |
445 |
423 |
0.00 |
8.21 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1199.8 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 1140.3 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 M06-2X/6-31G**
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.439 |
0.312 |
| S2 |
0.000 |
-1.439 |
0.312 |
| S3 |
-1.439 |
0.000 |
-0.312 |
| S4 |
1.439 |
0.000 |
-0.312 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8776 | 2.1285 | 2.1285 |
S2 | 2.8776 | | 2.1285 | 2.1285 | S3 | 2.1285 | 2.1285 | | 2.8776 | S4 | 2.1285 | 2.1285 | 2.8776 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.469 |
|
S1 |
S3 |
S4 |
47.469 |
| S2 |
S1 |
S3 |
47.469 |
|
S2 |
S4 |
S3 |
47.469 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/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 |
-50.031 |
0.000 |
0.000 |
| y |
0.000 |
-50.031 |
0.000 |
| z |
0.000 |
0.000 |
-55.202 |
|
| Traceless |
| | x | y | z |
| x |
2.585 |
0.000 |
0.000 |
| y |
0.000 |
2.585 |
0.000 |
| z |
0.000 |
0.000 |
-5.170 |
|
| Polar |
| 3z2-r2 | -10.341 |
| 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 |
10.499 |
0.000 |
0.000 |
| y |
0.000 |
10.499 |
0.000 |
| z |
0.000 |
0.000 |
5.332 |
<r2> (average value of r
2) Å
2
| <r2> |
171.058 |
| (<r2>)1/2 |
13.079 |
Jump to
S1C1
S1C3
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -1592.571013 |
| Energy at 298.15K | |
| HF Energy | -1592.571013 |
| Nuclear repulsion energy | 332.159074 |
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 M06-2X/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 |
690 |
656 |
2.99 |
32.82 |
0.20 |
0.33 |
| 2 |
A1 |
407 |
387 |
7.16 |
49.69 |
0.24 |
0.38 |
| 3 |
A1 |
125 |
118 |
0.58 |
14.99 |
0.47 |
0.64 |
| 4 |
A2 |
216 |
206 |
0.00 |
0.37 |
0.75 |
0.86 |
| 5 |
B2 |
663 |
630 |
176.53 |
3.56 |
0.75 |
0.86 |
| 6 |
B2 |
339 |
322 |
0.21 |
14.80 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1219.6 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 1159.1 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 M06-2X/6-31G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.047 |
0.917 |
| S2 |
0.000 |
-1.047 |
0.917 |
| S3 |
0.000 |
1.607 |
-0.917 |
| S4 |
0.000 |
-1.607 |
-0.917 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0933 | 1.9173 | 3.2258 |
S2 | 2.0933 | | 3.2258 | 1.9173 | S3 | 1.9173 | 3.2258 | | 3.2148 | S4 | 3.2258 | 1.9173 | 3.2148 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
107.005 |
|
S1 |
S3 |
S4 |
72.995 |
| S2 |
S1 |
S3 |
107.005 |
|
S2 |
S4 |
S3 |
72.995 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.115 |
|
|
|
| 2 |
S |
0.115 |
|
|
|
| 3 |
S |
-0.115 |
|
|
|
| 4 |
S |
-0.115 |
|
|
|
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 |
1.783 |
1.783 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.740 |
0.000 |
0.000 |
| y |
0.000 |
-54.739 |
0.000 |
| z |
0.000 |
0.000 |
-50.222 |
|
| Traceless |
| | x | y | z |
| x |
0.741 |
0.000 |
0.000 |
| y |
0.000 |
-3.758 |
0.000 |
| z |
0.000 |
0.000 |
3.017 |
|
| Polar |
| 3z2-r2 | 6.034 |
| x2-y2 | 3.000 |
| 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 |
4.372 |
0.000 |
0.000 |
| y |
0.000 |
18.712 |
0.000 |
| z |
0.000 |
0.000 |
11.031 |
<r2> (average value of r
2) Å
2
| <r2> |
204.145 |
| (<r2>)1/2 |
14.288 |
Jump to
S1C1
S1C2
Energy calculated at M06-2X/6-31G**
| | hartrees |
| Energy at 0K | -1592.564754 |
| Energy at 298.15K | |
| HF Energy | -1592.564754 |
| Nuclear repulsion energy | 335.924451 |
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 M06-2X/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 |
760 |
722 |
0.00 |
40.58 |
0.29 |
0.45 |
| 2 |
Ag |
314 |
299 |
0.00 |
49.26 |
0.30 |
0.46 |
| 3 |
Au |
256 |
243 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
698 |
664 |
199.43 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
139i |
132i |
24.69 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
346 |
329 |
0.00 |
18.34 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1117.4 cm
-1
Scaled (by 0.9504) Zero Point Vibrational Energy (zpe) 1062.0 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 M06-2X/6-31G**
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.947 |
1.265 |
| S2 |
0.000 |
0.947 |
-1.265 |
| S3 |
0.000 |
-0.947 |
1.265 |
| S4 |
0.000 |
-0.947 |
-1.265 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.5305 | 1.8931 | 3.1602 |
S2 | 2.5305 | | 3.1602 | 1.8931 | S3 | 1.8931 | 3.1602 | | 2.5305 | S4 | 3.1602 | 1.8931 | 2.5305 | |
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 M06-2X/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 |
-52.162 |
0.000 |
0.000 |
| y |
0.000 |
-49.548 |
0.000 |
| z |
0.000 |
0.000 |
-54.302 |
|
| Traceless |
| | x | y | z |
| x |
-0.237 |
0.000 |
0.000 |
| y |
0.000 |
3.684 |
0.000 |
| z |
0.000 |
0.000 |
-3.447 |
|
| Polar |
| 3z2-r2 | -6.895 |
| x2-y2 | -2.614 |
| 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 |
4.324 |
0.000 |
0.000 |
| y |
0.000 |
11.654 |
0.000 |
| z |
0.000 |
0.000 |
17.434 |
<r2> (average value of r
2) Å
2
| <r2> |
192.275 |
| (<r2>)1/2 |
13.866 |