Jump to
S1C2
S1C3
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -1592.702158 |
| Energy at 298.15K | |
| HF Energy | -1592.702158 |
| Nuclear repulsion energy | 343.489923 |
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 B3LYPultrafine/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 |
485 |
464 |
0.00 |
53.33 |
0.07 |
0.13 |
| 2 |
A1 |
188 |
180 |
0.00 |
3.12 |
0.75 |
0.86 |
| 3 |
B1 |
416 |
399 |
0.00 |
37.19 |
0.75 |
0.86 |
| 4 |
B2 |
304 |
291 |
0.26 |
12.18 |
0.75 |
0.86 |
| 5 |
E |
397 |
380 |
0.21 |
7.00 |
0.75 |
0.86 |
| 5 |
E |
397 |
380 |
0.21 |
7.00 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1093.3 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 1047.4 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 B3LYPultrafine/6-31G*
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.463 |
0.311 |
| S2 |
0.000 |
-1.463 |
0.311 |
| S3 |
-1.463 |
0.000 |
-0.311 |
| S4 |
1.463 |
0.000 |
-0.311 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9251 | 2.1600 | 2.1600 |
S2 | 2.9251 | | 2.1600 | 2.1600 | S3 | 2.1600 | 2.1600 | | 2.9251 | S4 | 2.1600 | 2.1600 | 2.9251 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.383 |
|
S1 |
S3 |
S4 |
47.383 |
| S2 |
S1 |
S3 |
47.383 |
|
S2 |
S4 |
S3 |
47.383 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/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 |
-49.757 |
0.000 |
0.000 |
| y |
0.000 |
-49.757 |
0.000 |
| z |
0.000 |
0.000 |
-55.100 |
|
| Traceless |
| | x | y | z |
| x |
2.672 |
0.000 |
0.000 |
| y |
0.000 |
2.672 |
0.000 |
| z |
0.000 |
0.000 |
-5.343 |
|
| Polar |
| 3z2-r2 | -10.687 |
| 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 |
10.732 |
0.000 |
0.000 |
| y |
0.000 |
10.732 |
0.000 |
| z |
0.000 |
0.000 |
5.320 |
<r2> (average value of r
2) Å
2
| <r2> |
175.292 |
| (<r2>)1/2 |
13.240 |
Jump to
S1C1
S1C3
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -1592.736433 |
| Energy at 298.15K | |
| HF Energy | -1592.736433 |
| Nuclear repulsion energy | 325.462820 |
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 B3LYPultrafine/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 |
662 |
634 |
2.01 |
31.40 |
0.24 |
0.38 |
| 2 |
A1 |
317 |
304 |
6.87 |
32.53 |
0.23 |
0.37 |
| 3 |
A1 |
95 |
91 |
1.18 |
9.47 |
0.51 |
0.67 |
| 4 |
A2 |
206 |
197 |
0.00 |
0.16 |
0.75 |
0.86 |
| 5 |
B2 |
640 |
613 |
122.36 |
2.56 |
0.75 |
0.86 |
| 6 |
B2 |
322 |
309 |
0.03 |
15.83 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1120.8 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 1073.7 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 B3LYPultrafine/6-31G*
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.098 |
0.932 |
| S2 |
0.000 |
-1.098 |
0.932 |
| S3 |
0.000 |
1.624 |
-0.932 |
| S4 |
0.000 |
-1.624 |
-0.932 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.1969 | 1.9359 | 3.2989 |
S2 | 2.1969 | | 3.2989 | 1.9359 | S3 | 1.9359 | 3.2989 | | 3.2477 | S4 | 3.2989 | 1.9359 | 3.2477 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
105.748 |
|
S1 |
S3 |
S4 |
74.252 |
| S2 |
S1 |
S3 |
105.748 |
|
S2 |
S4 |
S3 |
74.252 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYPultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.091 |
|
|
|
| 2 |
S |
0.091 |
|
|
|
| 3 |
S |
-0.091 |
|
|
|
| 4 |
S |
-0.091 |
|
|
|
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 |
1.446 |
1.446 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-51.593 |
0.000 |
0.000 |
| y |
0.000 |
-54.085 |
0.000 |
| z |
0.000 |
0.000 |
-49.831 |
|
| Traceless |
| | x | y | z |
| x |
0.365 |
0.000 |
0.000 |
| y |
0.000 |
-3.373 |
0.000 |
| z |
0.000 |
0.000 |
3.008 |
|
| Polar |
| 3z2-r2 | 6.016 |
| x2-y2 | 2.491 |
| 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 |
4.327 |
0.000 |
0.000 |
| y |
0.000 |
18.062 |
0.000 |
| z |
0.000 |
0.000 |
11.360 |
<r2> (average value of r
2) Å
2
| <r2> |
210.913 |
| (<r2>)1/2 |
14.523 |
Jump to
S1C1
S1C2
Energy calculated at B3LYPultrafine/6-31G*
| | hartrees |
| Energy at 0K | -1592.734065 |
| Energy at 298.15K | |
| HF Energy | -1592.734065 |
| Nuclear repulsion energy | 328.239206 |
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 B3LYPultrafine/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 |
707 |
677 |
0.00 |
38.05 |
0.28 |
0.44 |
| 2 |
Ag |
270 |
259 |
0.00 |
32.49 |
0.28 |
0.44 |
| 3 |
Au |
235 |
225 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
661 |
633 |
133.03 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
89i |
86i |
16.26 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
323 |
309 |
0.00 |
17.73 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1053.0 cm
-1
Scaled (by 0.958) Zero Point Vibrational Energy (zpe) 1008.8 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 B3LYPultrafine/6-31G*
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.960 |
1.307 |
| S2 |
0.000 |
0.960 |
-1.307 |
| S3 |
0.000 |
-0.960 |
1.307 |
| S4 |
0.000 |
-0.960 |
-1.307 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6140 | 1.9207 | 3.2438 |
S2 | 2.6140 | | 3.2438 | 1.9207 | S3 | 1.9207 | 3.2438 | | 2.6140 | S4 | 3.2438 | 1.9207 | 2.6140 | |
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 B3LYPultrafine/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 |
-51.905 |
0.000 |
0.000 |
| y |
0.000 |
-49.209 |
0.000 |
| z |
0.000 |
0.000 |
-53.684 |
|
| Traceless |
| | x | y | z |
| x |
-0.458 |
0.000 |
0.000 |
| y |
0.000 |
3.585 |
0.000 |
| z |
0.000 |
0.000 |
-3.127 |
|
| Polar |
| 3z2-r2 | -6.254 |
| x2-y2 | -2.696 |
| 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 |
4.288 |
0.000 |
0.000 |
| y |
0.000 |
11.906 |
0.000 |
| z |
0.000 |
0.000 |
17.112 |
<r2> (average value of r
2) Å
2
| <r2> |
200.581 |
| (<r2>)1/2 |
14.163 |