Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G
| hartrees |
Energy at 0K | -454.461156 |
Energy at 298.15K | -454.464734 |
HF Energy | -454.461156 |
Nuclear repulsion energy | 56.112362 |
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' |
3619 |
3462 |
11.81 |
|
|
|
2 |
A' |
2482 |
2375 |
84.86 |
|
|
|
3 |
A' |
1658 |
1586 |
16.48 |
|
|
|
4 |
A' |
986 |
943 |
7.16 |
|
|
|
5 |
A' |
821 |
785 |
53.19 |
|
|
|
6 |
A' |
385 |
369 |
239.29 |
|
|
|
7 |
A" |
3774 |
3610 |
27.62 |
|
|
|
8 |
A" |
1102 |
1054 |
7.36 |
|
|
|
9 |
A" |
509 |
487 |
71.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7668.2 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 7335.4 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 Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.027 |
1.139 |
0.000 |
S2 |
0.027 |
-0.641 |
0.000 |
H3 |
-1.341 |
-0.829 |
0.000 |
H4 |
0.362 |
1.552 |
0.856 |
H5 |
0.362 |
1.552 |
-0.856 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7796 | 2.3971 | 1.0076 | 1.0076 |
S2 | 1.7796 | | 1.3808 | 2.3771 | 2.3771 | H3 | 2.3971 | 1.3808 | | 3.0500 | 3.0500 | H4 | 1.0076 | 2.3771 | 3.0500 | | 1.7121 | H5 | 1.0076 | 2.3771 | 3.0500 | 1.7121 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.864 |
|
S2 |
N1 |
H4 |
114.170 |
S2 |
N1 |
H5 |
114.170 |
|
H4 |
N1 |
H5 |
116.333 |
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 |
N |
-0.912 |
|
|
|
2 |
S |
0.147 |
|
|
|
3 |
H |
0.077 |
|
|
|
4 |
H |
0.344 |
|
|
|
5 |
H |
0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.238 |
1.054 |
0.000 |
1.081 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.859 |
3.886 |
0.000 |
y |
3.886 |
-18.368 |
0.000 |
z |
0.000 |
0.000 |
-19.937 |
|
Traceless |
| x | y | z |
x |
-0.706 |
3.886 |
0.000 |
y |
3.886 |
1.530 |
0.000 |
z |
0.000 |
0.000 |
-0.824 |
|
Polar |
3z2-r2 | -1.648 |
x2-y2 | -1.491 |
xy | 3.886 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.906 |
0.617 |
0.000 |
y |
0.617 |
4.112 |
0.000 |
z |
0.000 |
0.000 |
2.292 |
<r2> (average value of r
2) Å
2
<r2> |
36.803 |
(<r2>)1/2 |
6.067 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G
| hartrees |
Energy at 0K | -454.461156 |
Energy at 298.15K | -454.464735 |
HF Energy | -454.461156 |
Nuclear repulsion energy | 56.112228 |
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' |
3619 |
3462 |
11.80 |
|
|
|
2 |
A' |
2482 |
2375 |
84.78 |
|
|
|
3 |
A' |
1658 |
1586 |
16.50 |
|
|
|
4 |
A' |
986 |
943 |
7.19 |
|
|
|
5 |
A' |
821 |
785 |
53.26 |
|
|
|
6 |
A' |
386 |
369 |
238.79 |
|
|
|
7 |
A" |
3774 |
3610 |
27.60 |
|
|
|
8 |
A" |
1103 |
1055 |
7.32 |
|
|
|
9 |
A" |
509 |
487 |
71.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7668.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 7335.6 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 HSEh1PBE/6-31G
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.027 |
1.139 |
0.000 |
S2 |
0.027 |
-0.640 |
0.000 |
H3 |
-1.341 |
-0.829 |
0.000 |
H4 |
0.362 |
1.551 |
0.856 |
H5 |
0.362 |
1.551 |
-0.856 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7797 | 2.3970 | 1.0077 | 1.0077 |
S2 | 1.7797 | | 1.3808 | 2.3769 | 2.3769 | H3 | 2.3970 | 1.3808 | | 3.0498 | 3.0498 | H4 | 1.0077 | 2.3769 | 3.0498 | | 1.7122 | H5 | 1.0077 | 2.3769 | 3.0498 | 1.7122 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
97.856 |
|
S2 |
N1 |
H4 |
114.149 |
S2 |
N1 |
H5 |
114.149 |
|
H4 |
N1 |
H5 |
116.339 |
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 |
N |
-0.912 |
|
|
|
2 |
S |
0.147 |
|
|
|
3 |
H |
0.077 |
|
|
|
4 |
H |
0.344 |
|
|
|
5 |
H |
0.344 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.239 |
1.054 |
0.000 |
1.080 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.857 |
3.888 |
0.000 |
y |
3.888 |
-18.372 |
0.000 |
z |
0.000 |
0.000 |
-19.937 |
|
Traceless |
| x | y | z |
x |
-0.703 |
3.888 |
0.000 |
y |
3.888 |
1.525 |
0.000 |
z |
0.000 |
0.000 |
-0.822 |
|
Polar |
3z2-r2 | -1.645 |
x2-y2 | -1.485 |
xy | 3.888 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
2.906 |
0.617 |
0.000 |
y |
0.617 |
4.112 |
0.000 |
z |
0.000 |
0.000 |
2.292 |
<r2> (average value of r
2) Å
2
<r2> |
36.802 |
(<r2>)1/2 |
6.066 |