Jump to
S1C2
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -1593.004215 |
| Energy at 298.15K | |
| HF Energy | -1593.004215 |
| Nuclear repulsion energy | 353.301623 |
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/cc-pVTZ
| 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 |
543 |
520 |
0.00 |
39.31 |
0.04 |
0.08 |
| 2 |
A1 |
211 |
202 |
0.00 |
2.41 |
0.74 |
0.85 |
| 3 |
B1 |
479 |
458 |
0.00 |
17.05 |
0.75 |
0.86 |
| 4 |
B2 |
301 |
288 |
0.00 |
8.35 |
0.75 |
0.86 |
| 5 |
E |
455 |
436 |
0.01 |
4.50 |
0.75 |
0.86 |
| 5 |
E |
455 |
436 |
0.01 |
4.50 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1222.0 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 1169.5 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/cc-pVTZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.416 |
0.323 |
| S2 |
0.000 |
-1.416 |
0.323 |
| S3 |
-1.416 |
0.000 |
-0.323 |
| S4 |
1.416 |
0.000 |
-0.323 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.8311 | 2.1035 | 2.1035 |
S2 | 2.8311 | | 2.1035 | 2.1035 | S3 | 2.1035 | 2.1035 | | 2.8311 | S4 | 2.1035 | 2.1035 | 2.8311 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.705 |
|
S1 |
S3 |
S4 |
47.705 |
| S2 |
S1 |
S3 |
47.705 |
|
S2 |
S4 |
S3 |
47.705 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
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 |
-48.477 |
0.000 |
0.000 |
| y |
0.000 |
-48.477 |
0.000 |
| z |
0.000 |
0.000 |
-53.743 |
|
| Traceless |
| | x | y | z |
| x |
2.633 |
0.000 |
0.000 |
| y |
0.000 |
2.633 |
0.000 |
| z |
0.000 |
0.000 |
-5.266 |
|
| Polar |
| 3z2-r2 | -10.532 |
| 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 |
11.207 |
0.000 |
0.000 |
| y |
0.000 |
11.207 |
0.000 |
| z |
0.000 |
0.000 |
6.641 |
<r2> (average value of r
2) Å
2
| <r2> |
166.295 |
| (<r2>)1/2 |
12.896 |
Jump to
S1C1
S1C3
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -1593.024757 |
| Energy at 298.15K | |
| HF Energy | -1593.024757 |
| Nuclear repulsion energy | 335.200026 |
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/cc-pVTZ
| 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 |
705 |
675 |
6.03 |
26.36 |
0.15 |
0.26 |
| 2 |
A1 |
406 |
388 |
6.01 |
39.51 |
0.19 |
0.32 |
| 3 |
A1 |
119 |
114 |
0.59 |
10.40 |
0.44 |
0.61 |
| 4 |
A2 |
221 |
211 |
0.00 |
0.12 |
0.75 |
0.86 |
| 5 |
B2 |
675 |
646 |
122.23 |
3.33 |
0.75 |
0.86 |
| 6 |
B2 |
340 |
326 |
0.19 |
11.42 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1232.7 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 1179.8 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 B1B95/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.046 |
0.914 |
| S2 |
0.000 |
-1.046 |
0.914 |
| S3 |
0.000 |
1.570 |
-0.914 |
| S4 |
0.000 |
-1.570 |
-0.914 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.0910 | 1.9027 | 3.1918 |
S2 | 2.0910 | | 3.1918 | 1.9027 | S3 | 1.9027 | 3.1918 | | 3.1407 | S4 | 3.1918 | 1.9027 | 3.1407 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
106.011 |
|
S1 |
S3 |
S4 |
73.989 |
| S2 |
S1 |
S3 |
106.011 |
|
S2 |
S4 |
S3 |
73.989 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
S |
0.134 |
|
|
|
| 2 |
S |
0.134 |
|
|
|
| 3 |
S |
-0.134 |
|
|
|
| 4 |
S |
-0.134 |
|
|
|
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 |
1.447 |
1.447 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-50.844 |
0.000 |
0.000 |
| y |
0.000 |
-52.826 |
0.000 |
| z |
0.000 |
0.000 |
-48.081 |
|
| Traceless |
| | x | y | z |
| x |
-0.391 |
0.000 |
0.000 |
| y |
0.000 |
-3.363 |
0.000 |
| z |
0.000 |
0.000 |
3.754 |
|
| Polar |
| 3z2-r2 | 7.508 |
| x2-y2 | 1.981 |
| 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 |
5.774 |
0.000 |
0.000 |
| y |
0.000 |
17.991 |
0.000 |
| z |
0.000 |
0.000 |
11.765 |
<r2> (average value of r
2) Å
2
| <r2> |
199.003 |
| (<r2>)1/2 |
14.107 |
Jump to
S1C1
S1C2
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -1593.018446 |
| Energy at 298.15K | |
| HF Energy | -1593.018446 |
| Nuclear repulsion energy | 338.924991 |
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/cc-pVTZ
| 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 |
761 |
728 |
0.00 |
33.09 |
0.20 |
0.33 |
| 2 |
Ag |
308 |
295 |
0.00 |
37.22 |
0.24 |
0.39 |
| 3 |
Au |
257 |
246 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
701 |
671 |
129.97 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
160i |
153i |
18.70 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
345 |
330 |
0.00 |
13.06 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 1106.1 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 1058.6 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/cc-pVTZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
0.942 |
1.249 |
| S2 |
0.000 |
0.942 |
-1.249 |
| S3 |
0.000 |
-0.942 |
1.249 |
| S4 |
0.000 |
-0.942 |
-1.249 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.4979 | 1.8834 | 3.1284 |
S2 | 2.4979 | | 3.1284 | 1.8834 | S3 | 1.8834 | 3.1284 | | 2.4979 | S4 | 3.1284 | 1.8834 | 2.4979 | |
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/cc-pVTZ
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 |
-51.169 |
0.000 |
0.000 |
| y |
0.000 |
-47.465 |
0.000 |
| z |
0.000 |
0.000 |
-52.363 |
|
| Traceless |
| | x | y | z |
| x |
-1.255 |
0.000 |
0.000 |
| y |
0.000 |
4.301 |
0.000 |
| z |
0.000 |
0.000 |
-3.046 |
|
| Polar |
| 3z2-r2 | -6.092 |
| x2-y2 | -3.704 |
| 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 |
5.755 |
0.000 |
0.000 |
| y |
0.000 |
12.247 |
0.000 |
| z |
0.000 |
0.000 |
17.097 |
<r2> (average value of r
2) Å
2
| <r2> |
188.027 |
| (<r2>)1/2 |
13.712 |