Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G**
| hartrees |
Energy at 0K | -1195.353881 |
Energy at 298.15K | -1195.356284 |
HF Energy | -1195.353881 |
Nuclear repulsion energy | 194.651760 |
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 HSEh1PBE/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 |
A |
2691 |
2568 |
0.77 |
|
|
|
2 |
A |
894 |
853 |
0.83 |
|
|
|
3 |
A |
497 |
474 |
0.84 |
|
|
|
4 |
A |
334 |
318 |
32.24 |
|
|
|
5 |
A |
208 |
199 |
0.10 |
|
|
|
6 |
B |
2690 |
2567 |
11.93 |
|
|
|
7 |
B |
879 |
839 |
14.89 |
|
|
|
8 |
B |
484 |
462 |
31.88 |
|
|
|
9 |
B |
359 |
343 |
23.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4517.9 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 4311.4 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 HSEh1PBE/6-31G**
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
0.000 |
0.000 |
0.830 |
S2 |
0.000 |
1.682 |
-0.379 |
S3 |
0.000 |
-1.682 |
-0.379 |
H4 |
-1.331 |
1.795 |
-0.577 |
H5 |
1.331 |
-1.795 |
-0.577 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0719 | 2.0719 | 2.6410 | 2.6410 |
S2 | 2.0719 | | 3.3644 | 1.3500 | 3.7287 | S3 | 2.0719 | 3.3644 | | 3.7287 | 1.3500 | H4 | 2.6410 | 1.3500 | 3.7287 | | 4.4694 | H5 | 2.6410 | 3.7287 | 1.3500 | 4.4694 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.842 |
|
S1 |
S3 |
H5 |
98.842 |
S2 |
S1 |
S3 |
108.568 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.057 |
|
|
|
2 |
S |
-0.080 |
|
|
|
3 |
S |
-0.080 |
|
|
|
4 |
H |
0.108 |
|
|
|
5 |
H |
0.108 |
|
|
|
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 |
-0.716 |
0.716 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.291 |
-4.593 |
0.000 |
y |
-4.593 |
-39.723 |
0.000 |
z |
0.000 |
0.000 |
-41.917 |
|
Traceless |
| x | y | z |
x |
3.529 |
-4.593 |
0.000 |
y |
-4.593 |
-0.119 |
0.000 |
z |
0.000 |
0.000 |
-3.410 |
|
Polar |
3z2-r2 | -6.820 |
x2-y2 | 2.432 |
xy | -4.593 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.446 |
-0.701 |
0.000 |
y |
-0.701 |
11.101 |
0.000 |
z |
0.000 |
0.000 |
5.863 |
<r2> (average value of r
2) Å
2
<r2> |
141.598 |
(<r2>)1/2 |
11.899 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G**
| hartrees |
Energy at 0K | -1195.353435 |
Energy at 298.15K | -1195.355805 |
HF Energy | -1195.353435 |
Nuclear repulsion energy | 194.661883 |
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 HSEh1PBE/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 |
A' |
2678 |
2556 |
17.59 |
|
|
|
2 |
A' |
893 |
852 |
7.37 |
|
|
|
3 |
A' |
497 |
474 |
0.81 |
|
|
|
4 |
A' |
341 |
325 |
23.98 |
|
|
|
5 |
A' |
209 |
199 |
0.24 |
|
|
|
6 |
A" |
2680 |
2557 |
1.02 |
|
|
|
7 |
A" |
882 |
842 |
10.18 |
|
|
|
8 |
A" |
485 |
463 |
36.13 |
|
|
|
9 |
A" |
320 |
305 |
11.53 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4492.1 cm
-1
Scaled (by 0.9543) Zero Point Vibrational Energy (zpe) 4286.8 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 HSEh1PBE/6-31G**
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
S1 |
-0.053 |
0.828 |
0.000 |
S2 |
-0.053 |
-0.382 |
1.682 |
S3 |
-0.053 |
-0.382 |
-1.682 |
H4 |
1.281 |
-0.511 |
1.843 |
H5 |
1.281 |
-0.511 |
-1.843 |
Atom - Atom Distances (Å)
|
S1 |
S2 |
S3 |
H4 |
H5 |
S1 | | 2.0714 | 2.0714 | 2.6402 | 2.6402 |
S2 | 2.0714 | | 3.3633 | 1.3505 | 3.7713 | S3 | 2.0714 | 3.3633 | | 3.7713 | 1.3505 | H4 | 2.6402 | 1.3505 | 3.7713 | | 3.6865 | H5 | 2.6402 | 3.7713 | 1.3505 | 3.6865 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
S1 |
S2 |
H4 |
98.800 |
|
S1 |
S3 |
H5 |
98.800 |
S2 |
S1 |
S3 |
108.551 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
S |
-0.057 |
|
|
|
2 |
S |
-0.072 |
|
|
|
3 |
S |
-0.072 |
|
|
|
4 |
H |
0.100 |
|
|
|
5 |
H |
0.100 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
2.172 |
-0.596 |
0.000 |
2.252 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-37.557 |
-1.558 |
0.000 |
y |
-1.558 |
-42.083 |
0.000 |
z |
0.000 |
0.000 |
-39.417 |
|
Traceless |
| x | y | z |
x |
3.193 |
-1.558 |
0.000 |
y |
-1.558 |
-3.596 |
0.000 |
z |
0.000 |
0.000 |
0.403 |
|
Polar |
3z2-r2 | 0.806 |
x2-y2 | 4.526 |
xy | -1.558 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
5.421 |
-0.327 |
0.000 |
y |
-0.327 |
5.821 |
0.000 |
z |
0.000 |
0.000 |
11.137 |
<r2> (average value of r
2) Å
2
<r2> |
141.645 |
(<r2>)1/2 |
11.901 |