Jump to
S1C2
S1C3
Energy calculated at B2PLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.175548 |
| Energy at 298.15K | |
| HF Energy | -1592.001212 |
| Nuclear repulsion energy | 343.775843 |
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 B2PLYP/cc-pVDZ
| 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 |
499 |
478 |
0.00 |
41.69 |
0.06 |
0.10 |
| 2 |
A1 |
190 |
182 |
0.00 |
3.68 |
0.75 |
0.86 |
| 3 |
B1 |
435 |
417 |
0.00 |
23.84 |
0.75 |
0.86 |
| 4 |
B2 |
303 |
291 |
0.04 |
11.35 |
0.75 |
0.86 |
| 5 |
E |
411 |
394 |
0.12 |
5.81 |
0.75 |
0.86 |
| 5 |
E |
411 |
394 |
0.12 |
5.81 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1124.9 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1077.3 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 B2PLYP/cc-pVDZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.460 |
0.317 |
| S2 |
0.000 |
-1.460 |
0.317 |
| S3 |
-1.460 |
0.000 |
-0.317 |
| S4 |
1.460 |
0.000 |
-0.317 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.9192 | 2.1592 | 2.1592 |
S2 | 2.9192 | | 2.1592 | 2.1592 | S3 | 2.1592 | 2.1592 | | 2.9192 | S4 | 2.1592 | 2.1592 | 2.9192 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.470 |
|
S1 |
S3 |
S4 |
47.470 |
| S2 |
S1 |
S3 |
47.470 |
|
S2 |
S4 |
S3 |
47.470 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
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 |
-49.170 |
0.000 |
0.000 |
| y |
0.000 |
-49.126 |
0.000 |
| z |
0.000 |
0.000 |
-54.810 |
|
| Traceless |
| | x | y | z |
| x |
2.798 |
0.000 |
0.000 |
| y |
0.000 |
2.863 |
0.000 |
| z |
0.000 |
0.000 |
-5.662 |
|
| Polar |
| 3z2-r2 | -11.323 |
| x2-y2 | -0.043 |
| 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 |
10.413 |
0.000 |
0.000 |
| y |
0.000 |
10.412 |
0.000 |
| z |
0.000 |
0.000 |
4.992 |
<r2> (average value of r
2) Å
2
| <r2> |
174.642 |
| (<r2>)1/2 |
13.215 |
Jump to
S1C1
S1C3
Energy calculated at B2PLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.219074 |
| Energy at 298.15K | |
| HF Energy | -1591.992442 |
| Nuclear repulsion energy | 323.736307 |
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 B2PLYP/cc-pVDZ
| 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 |
678 |
649 |
0.00 |
33.71 |
0.20 |
0.33 |
| 2 |
A1 |
229 |
219 |
0.00 |
15.00 |
0.50 |
0.67 |
| 3 |
A1 |
123 |
117 |
6.50 |
0.00 |
0.31 |
0.47 |
| 4 |
A2 |
218 |
209 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
665 |
637 |
37.11 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
304 |
291 |
0.00 |
16.54 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1108.0 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1061.1 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 B2PLYP/cc-pVDZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.332 |
0.969 |
| S2 |
0.000 |
-1.332 |
0.969 |
| S3 |
0.000 |
1.333 |
-0.969 |
| S4 |
0.000 |
-1.333 |
-0.969 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6649 | 1.9375 | 3.2948 |
S2 | 2.6649 | | 3.2948 | 1.9375 | S3 | 1.9375 | 3.2948 | | 2.6650 | S4 | 3.2948 | 1.9375 | 2.6650 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
90.002 |
|
S1 |
S3 |
S4 |
89.998 |
| S2 |
S1 |
S3 |
90.002 |
|
S2 |
S4 |
S3 |
89.998 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP/cc-pVDZ
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 |
-51.703 |
0.000 |
0.000 |
| y |
0.000 |
-52.922 |
0.000 |
| z |
0.000 |
0.000 |
-48.235 |
|
| Traceless |
| | x | y | z |
| x |
-1.125 |
0.000 |
0.000 |
| y |
0.000 |
-2.953 |
0.000 |
| z |
0.000 |
0.000 |
4.078 |
|
| Polar |
| 3z2-r2 | 8.155 |
| x2-y2 | 1.219 |
| 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 |
4.101 |
0.000 |
0.000 |
| y |
0.000 |
13.966 |
0.000 |
| z |
0.000 |
0.000 |
11.785 |
<r2> (average value of r
2) Å
2
| <r2> |
205.520 |
| (<r2>)1/2 |
14.336 |
Jump to
S1C1
S1C2
Energy calculated at B2PLYP/cc-pVDZ
| | hartrees |
| Energy at 0K | -1592.219074 |
| Energy at 298.15K | |
| HF Energy | -1591.992427 |
| Nuclear repulsion energy | 323.723581 |
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 B2PLYP/cc-pVDZ
| 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 |
678 |
649 |
0.00 |
33.70 |
0.20 |
0.33 |
| 2 |
Ag |
229 |
220 |
0.00 |
14.90 |
0.50 |
0.67 |
| 3 |
Au |
218 |
209 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
664 |
636 |
37.09 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
123 |
118 |
6.51 |
0.00 |
0.33 |
0.50 |
| 6 |
B3g |
304 |
291 |
0.00 |
16.54 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1107.8 cm
-1
Scaled (by 0.9577) Zero Point Vibrational Energy (zpe) 1060.9 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 B2PLYP/cc-pVDZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.969 |
1.332 |
| S2 |
0.000 |
0.969 |
-1.332 |
| S3 |
0.000 |
-0.969 |
1.332 |
| S4 |
0.000 |
-0.969 |
-1.332 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.6648 | 1.9378 | 3.2949 |
S2 | 2.6648 | | 3.2949 | 1.9378 | S3 | 1.9378 | 3.2949 | | 2.6648 | S4 | 3.2949 | 1.9378 | 2.6648 | |
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 B2PLYP/cc-pVDZ
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 |
-51.704 |
0.000 |
0.000 |
| y |
0.000 |
-48.233 |
0.000 |
| z |
0.000 |
0.000 |
-52.924 |
|
| Traceless |
| | x | y | z |
| x |
-1.126 |
0.000 |
0.000 |
| y |
0.000 |
4.081 |
0.000 |
| z |
0.000 |
0.000 |
-2.955 |
|
| Polar |
| 3z2-r2 | -5.911 |
| x2-y2 | -3.471 |
| 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 |
4.101 |
0.000 |
0.000 |
| y |
0.000 |
11.787 |
0.000 |
| z |
0.000 |
0.000 |
13.969 |
<r2> (average value of r
2) Å
2
| <r2> |
205.521 |
| (<r2>)1/2 |
14.336 |