Jump to
S1C2
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.465763 |
| Energy at 298.15K | -491.466535 |
| HF Energy | -491.465763 |
| Nuclear repulsion energy | 80.071880 |
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-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 |
A' |
3714 |
3570 |
255.15 |
|
|
|
| 2 |
A' |
2081 |
2000 |
726.38 |
|
|
|
| 3 |
A' |
895 |
860 |
3.25 |
|
|
|
| 4 |
A' |
638 |
613 |
321.41 |
|
|
|
| 5 |
A' |
463 |
445 |
97.14 |
|
|
|
| 6 |
A" |
499 |
480 |
1.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4144.5 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 3983.3 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-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
-0.139 |
1.683 |
0.000 |
| C2 |
0.000 |
0.494 |
0.000 |
| S3 |
0.028 |
-1.074 |
0.000 |
| H4 |
0.523 |
2.437 |
0.000 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1973 | 2.7623 | 1.0031 |
C2 | 1.1973 | | 1.5682 | 2.0122 | S3 | 2.7623 | 1.5682 | | 3.5457 | H4 | 1.0031 | 2.0122 | 3.5457 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
174.376 |
|
C2 |
N1 |
H4 |
132.067 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.148 |
|
|
|
| 2 |
C |
0.080 |
|
|
|
| 3 |
S |
-0.139 |
|
|
|
| 4 |
H |
0.206 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.118 |
1.723 |
0.000 |
2.054 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.274 |
2.989 |
0.000 |
| y |
2.989 |
-19.182 |
0.000 |
| z |
0.000 |
0.000 |
-25.125 |
|
| Traceless |
| | x | y | z |
| x |
-2.120 |
2.989 |
0.000 |
| y |
2.989 |
5.518 |
0.000 |
| z |
0.000 |
0.000 |
-3.397 |
|
| Polar |
| 3z2-r2 | -6.795 |
| x2-y2 | -5.092 |
| xy | 2.989 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.223 |
-0.153 |
0.000 |
| y |
-0.153 |
9.134 |
0.000 |
| z |
0.000 |
0.000 |
3.095 |
<r2> (average value of r
2) Å
2
| <r2> |
60.390 |
| (<r2>)1/2 |
7.771 |
Jump to
S1C1
Energy calculated at HSEh1PBE/cc-pVTZ
| | hartrees |
| Energy at 0K | -491.462222 |
| Energy at 298.15K | |
| HF Energy | -491.462222 |
| Nuclear repulsion energy | 80.102395 |
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-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 |
Σ |
3924 |
3771 |
715.78 |
|
|
|
| 2 |
Σ |
2190 |
2105 |
748.10 |
|
|
|
| 3 |
Σ |
875 |
841 |
29.11 |
|
|
|
| 4 |
Π |
495 |
476 |
6.18 |
|
|
|
| 4 |
Π |
495 |
476 |
6.18 |
|
|
|
| 5 |
Π |
452i |
434i |
147.59 |
|
|
|
| 5 |
Π |
452i |
434i |
147.59 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3537.1 cm
-1
Scaled (by 0.9611) Zero Point Vibrational Energy (zpe) 3399.5 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 HSEh1PBE/cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
-1.670 |
| C2 |
0.000 |
0.000 |
-0.496 |
| S3 |
0.000 |
0.000 |
1.083 |
| H4 |
0.000 |
0.000 |
-2.659 |
Atom - Atom Distances (Å)
| |
N1 |
C2 |
S3 |
H4 |
| N1 | | 1.1740 | 2.7532 | 0.9890 |
C2 | 1.1740 | | 1.5793 | 2.1630 | S3 | 2.7532 | 1.5793 | | 3.7422 | H4 | 0.9890 | 2.1630 | 3.7422 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| N1 |
C2 |
S3 |
180.000 |
|
C2 |
N1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.135 |
|
|
|
| 2 |
C |
0.095 |
|
|
|
| 3 |
S |
-0.194 |
|
|
|
| 4 |
H |
0.235 |
|
|
|
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 |
-3.072 |
3.072 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.094 |
0.000 |
0.000 |
| y |
0.000 |
-25.094 |
0.000 |
| z |
0.000 |
0.000 |
-15.755 |
|
| Traceless |
| | x | y | z |
| x |
-4.669 |
0.000 |
0.000 |
| y |
0.000 |
-4.669 |
0.000 |
| z |
0.000 |
0.000 |
9.339 |
|
| Polar |
| 3z2-r2 | 18.677 |
| 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 |
3.075 |
0.000 |
0.000 |
| y |
0.000 |
3.075 |
0.000 |
| z |
0.000 |
0.000 |
8.938 |
<r2> (average value of r
2) Å
2
| <r2> |
60.571 |
| (<r2>)1/2 |
7.783 |