Jump to
S1C2
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -40.329786 |
| Energy at 298.15K | |
| HF Energy | -40.329786 |
| Nuclear repulsion energy | 43.940990 |
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/LANL2DZ
| 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 |
423 |
406 |
0.00 |
46.44 |
0.06 |
0.11 |
| 2 |
A1 |
142 |
136 |
0.00 |
13.83 |
0.73 |
0.84 |
| 3 |
B1 |
335 |
322 |
0.00 |
29.24 |
0.75 |
0.86 |
| 4 |
B2 |
257 |
247 |
0.08 |
17.76 |
0.75 |
0.86 |
| 5 |
E |
328 |
315 |
0.11 |
9.05 |
0.75 |
0.86 |
| 5 |
E |
328 |
315 |
0.11 |
9.05 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 905.3 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 870.1 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/LANL2DZ
Point Group is D2d
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.607 |
0.345 |
| S2 |
0.000 |
-1.607 |
0.345 |
| S3 |
-1.607 |
0.000 |
-0.345 |
| S4 |
1.607 |
0.000 |
-0.345 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 3.2139 | 2.3749 | 2.3749 |
S2 | 3.2139 | | 2.3749 | 2.3749 | S3 | 2.3749 | 2.3749 | | 3.2139 | S4 | 2.3749 | 2.3749 | 3.2139 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
47.420 |
|
S1 |
S3 |
S4 |
47.420 |
| S2 |
S1 |
S3 |
47.420 |
|
S2 |
S4 |
S3 |
47.420 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
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 |
-49.127 |
0.000 |
0.000 |
| y |
0.000 |
-49.127 |
0.000 |
| z |
0.000 |
0.000 |
-53.784 |
|
| Traceless |
| | x | y | z |
| x |
2.328 |
0.000 |
0.000 |
| y |
0.000 |
2.328 |
0.000 |
| z |
0.000 |
0.000 |
-4.657 |
|
| Polar |
| 3z2-r2 | -9.314 |
| 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 |
12.840 |
0.000 |
0.000 |
| y |
0.000 |
12.840 |
0.000 |
| z |
0.000 |
0.000 |
2.670 |
<r2> (average value of r
2) Å
2
| <r2> |
96.482 |
| (<r2>)1/2 |
9.823 |
Jump to
S1C1
S1C3
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -40.351078 |
| Energy at 298.15K | |
| HF Energy | -40.351078 |
| Nuclear repulsion energy | 42.977752 |
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/LANL2DZ
| 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 |
569 |
547 |
0.00 |
32.77 |
0.27 |
0.43 |
| 2 |
A1 |
270 |
260 |
0.00 |
27.75 |
0.26 |
0.42 |
| 3 |
A1 |
86 |
83 |
6.32 |
0.00 |
0.54 |
0.70 |
| 4 |
A2 |
187 |
180 |
0.00 |
0.00 |
0.75 |
0.86 |
| 5 |
B2 |
540 |
519 |
81.73 |
0.00 |
0.75 |
0.86 |
| 6 |
B2 |
262 |
252 |
0.00 |
22.76 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 957.2 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 920.1 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/LANL2DZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.385 |
1.044 |
| S2 |
0.000 |
-1.385 |
1.044 |
| S3 |
0.000 |
1.385 |
-1.044 |
| S4 |
0.000 |
-1.385 |
-1.044 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7700 | 2.0888 | 3.4693 |
S2 | 2.7700 | | 3.4693 | 2.0888 | S3 | 2.0888 | 3.4693 | | 2.7700 | S4 | 3.4693 | 2.0888 | 2.7700 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| S1 |
S2 |
S4 |
89.999 |
|
S1 |
S3 |
S4 |
90.001 |
| S2 |
S1 |
S3 |
89.999 |
|
S2 |
S4 |
S3 |
90.001 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3LYP/LANL2DZ
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 |
-50.219 |
0.000 |
0.000 |
| y |
0.000 |
-52.776 |
0.000 |
| z |
0.000 |
0.000 |
-48.942 |
|
| Traceless |
| | x | y | z |
| x |
0.640 |
0.000 |
0.000 |
| y |
0.000 |
-3.196 |
0.000 |
| z |
0.000 |
0.000 |
2.556 |
|
| Polar |
| 3z2-r2 | 5.112 |
| x2-y2 | 2.557 |
| 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 |
1.659 |
0.000 |
0.000 |
| y |
0.000 |
16.969 |
0.000 |
| z |
0.000 |
0.000 |
13.195 |
<r2> (average value of r
2) Å
2
| <r2> |
103.848 |
| (<r2>)1/2 |
10.191 |
Jump to
S1C1
S1C2
Energy calculated at B3LYP/LANL2DZ
| | hartrees |
| Energy at 0K | -40.351078 |
| Energy at 298.15K | |
| HF Energy | -40.351078 |
| Nuclear repulsion energy | 42.981561 |
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/LANL2DZ
| 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 |
570 |
548 |
0.00 |
32.78 |
0.27 |
0.43 |
| 2 |
Ag |
270 |
260 |
0.00 |
27.75 |
0.26 |
0.42 |
| 3 |
Au |
187 |
180 |
0.00 |
0.00 |
0.00 |
0.00 |
| 4 |
B1u |
540 |
519 |
81.84 |
0.00 |
0.00 |
0.00 |
| 5 |
B2u |
86 |
82 |
6.32 |
0.00 |
0.00 |
0.00 |
| 6 |
B3g |
262 |
252 |
0.00 |
22.75 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 957.5 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 920.3 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 B3LYP/LANL2DZ
Point Group is D2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| S1 |
0.000 |
1.044 |
1.385 |
| S2 |
0.000 |
1.044 |
-1.385 |
| S3 |
0.000 |
-1.044 |
1.385 |
| S4 |
0.000 |
-1.044 |
-1.385 |
Atom - Atom Distances (Å)
| |
S1 |
S2 |
S3 |
S4 |
| S1 | | 2.7701 | 2.0884 | 3.4691 |
S2 | 2.7701 | | 3.4691 | 2.0884 | S3 | 2.0884 | 3.4691 | | 2.7701 | S4 | 3.4691 | 2.0884 | 2.7701 | |
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/LANL2DZ
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 |
-50.218 |
0.000 |
0.000 |
| y |
0.000 |
-48.945 |
0.000 |
| z |
0.000 |
0.000 |
-52.774 |
|
| Traceless |
| | x | y | z |
| x |
0.642 |
0.000 |
0.000 |
| y |
0.000 |
2.551 |
0.000 |
| z |
0.000 |
0.000 |
-3.192 |
|
| Polar |
| 3z2-r2 | -6.385 |
| x2-y2 | -1.273 |
| 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 |
1.659 |
0.000 |
0.000 |
| y |
0.000 |
13.191 |
0.000 |
| z |
0.000 |
0.000 |
16.969 |
<r2> (average value of r
2) Å
2
| <r2> |
103.840 |
| (<r2>)1/2 |
10.190 |