Jump to
S1C2
Energy calculated at HSEh1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -454.541969 |
Energy at 298.15K | -454.545711 |
HF Energy | -454.541969 |
Nuclear repulsion energy | 57.287480 |
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/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 |
A' |
3510 |
3376 |
5.62 |
|
|
|
2 |
A' |
2663 |
2561 |
17.31 |
|
|
|
3 |
A' |
1612 |
1551 |
11.67 |
|
|
|
4 |
A' |
1028 |
989 |
11.92 |
|
|
|
5 |
A' |
902 |
867 |
40.53 |
|
|
|
6 |
A' |
674 |
648 |
51.34 |
|
|
|
7 |
A" |
3606 |
3469 |
15.14 |
|
|
|
8 |
A" |
1134 |
1090 |
0.92 |
|
|
|
9 |
A" |
409 |
394 |
64.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7768.6 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 7472.6 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/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.012 |
1.119 |
0.000 |
S2 |
0.012 |
-0.620 |
0.000 |
H3 |
-1.338 |
-0.780 |
0.000 |
H4 |
0.530 |
1.432 |
0.821 |
H5 |
0.530 |
1.432 |
-0.821 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7394 | 2.3306 | 1.0199 | 1.0199 |
S2 | 1.7394 | | 1.3597 | 2.2699 | 2.2699 | H3 | 2.3306 | 1.3597 | | 3.0095 | 3.0095 | H4 | 1.0199 | 2.2699 | 3.0095 | | 1.6425 | H5 | 1.0199 | 2.2699 | 3.0095 | 1.6425 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
96.769 |
|
S2 |
N1 |
H4 |
107.838 |
S2 |
N1 |
H5 |
107.838 |
|
H4 |
N1 |
H5 |
107.266 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.315 |
|
|
|
2 |
S |
-0.047 |
|
|
|
3 |
H |
0.101 |
|
|
|
4 |
H |
0.131 |
|
|
|
5 |
H |
0.131 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.554 |
0.793 |
0.000 |
0.967 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-18.535 |
3.651 |
0.000 |
y |
3.651 |
-18.936 |
0.000 |
z |
0.000 |
0.000 |
-20.006 |
|
Traceless |
| x | y | z |
x |
0.936 |
3.651 |
0.000 |
y |
3.651 |
0.335 |
0.000 |
z |
0.000 |
0.000 |
-1.271 |
|
Polar |
3z2-r2 | -2.541 |
x2-y2 | 0.401 |
xy | 3.651 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.289 |
0.555 |
0.000 |
y |
0.555 |
4.207 |
0.000 |
z |
0.000 |
0.000 |
2.439 |
<r2> (average value of r
2) Å
2
<r2> |
35.302 |
(<r2>)1/2 |
5.942 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVDZ
| hartrees |
Energy at 0K | -454.541177 |
Energy at 298.15K | -454.544994 |
HF Energy | -454.541177 |
Nuclear repulsion energy | 57.584541 |
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/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 |
A' |
3518 |
3384 |
2.46 |
|
|
|
2 |
A' |
2562 |
2465 |
59.40 |
|
|
|
3 |
A' |
1595 |
1534 |
14.23 |
|
|
|
4 |
A' |
1016 |
978 |
30.16 |
|
|
|
5 |
A' |
891 |
857 |
16.36 |
|
|
|
6 |
A' |
649 |
624 |
113.36 |
|
|
|
7 |
A" |
3625 |
3486 |
16.68 |
|
|
|
8 |
A" |
1115 |
1072 |
1.35 |
|
|
|
9 |
A" |
523 |
503 |
3.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7746.4 cm
-1
Scaled (by 0.9619) Zero Point Vibrational Energy (zpe) 7451.3 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 HSEh1PBE/cc-pVDZ
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.087 |
1.106 |
0.000 |
S2 |
0.087 |
-0.611 |
0.000 |
H3 |
-1.248 |
-0.923 |
0.000 |
H4 |
-0.373 |
1.478 |
0.829 |
H5 |
-0.373 |
1.478 |
-0.829 |
Atom - Atom Distances (Å)
|
N1 |
S2 |
H3 |
H4 |
H5 |
N1 | | 1.7172 | 2.4287 | 1.0185 | 1.0185 |
S2 | 1.7172 | | 1.3710 | 2.2938 | 2.2938 | H3 | 2.4287 | 1.3710 | | 2.6860 | 2.6860 | H4 | 1.0185 | 2.2938 | 2.6860 | | 1.6589 | H5 | 1.0185 | 2.2938 | 2.6860 | 1.6589 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
S2 |
H3 |
103.138 |
|
S2 |
N1 |
H4 |
111.381 |
S2 |
N1 |
H5 |
111.381 |
|
H4 |
N1 |
H5 |
109.053 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.308 |
|
|
|
2 |
S |
-0.014 |
|
|
|
3 |
H |
0.064 |
|
|
|
4 |
H |
0.129 |
|
|
|
5 |
H |
0.129 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-2.187 |
0.950 |
0.000 |
2.385 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-19.547 |
-1.157 |
0.000 |
y |
-1.157 |
-18.176 |
0.000 |
z |
0.000 |
0.000 |
-19.927 |
|
Traceless |
| x | y | z |
x |
-0.496 |
-1.157 |
0.000 |
y |
-1.157 |
1.561 |
0.000 |
z |
0.000 |
0.000 |
-1.065 |
|
Polar |
3z2-r2 | -2.130 |
x2-y2 | -1.371 |
xy | -1.157 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
3.233 |
0.281 |
0.000 |
y |
0.281 |
4.211 |
0.000 |
z |
0.000 |
0.000 |
2.438 |
<r2> (average value of r
2) Å
2
<r2> |
35.145 |
(<r2>)1/2 |
5.928 |