Jump to
S1C2
Energy calculated at HSEh1PBE/6-31G
| hartrees |
Energy at 0K | -491.334794 |
Energy at 298.15K | -491.335114 |
HF Energy | -491.334794 |
Nuclear repulsion energy | 78.414138 |
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' |
3932 |
3761 |
591.80 |
|
|
|
2 |
A' |
2182 |
2087 |
570.66 |
|
|
|
3 |
A' |
804 |
769 |
19.56 |
|
|
|
4 |
A' |
440 |
421 |
1.64 |
|
|
|
5 |
A' |
250 |
239 |
319.67 |
|
|
|
6 |
A" |
441 |
422 |
2.95 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4024.3 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3849.7 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 |
-0.074 |
1.706 |
0.000 |
C2 |
0.000 |
0.520 |
0.000 |
S3 |
0.021 |
-1.108 |
0.000 |
H4 |
0.186 |
2.664 |
0.000 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
S3 |
H4 |
N1 | | 1.1882 | 2.8152 | 0.9926 |
C2 | 1.1882 | | 1.6278 | 2.1522 | S3 | 2.8152 | 1.6278 | | 3.7755 | H4 | 0.9926 | 2.1522 | 3.7755 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
N1 |
C2 |
S3 |
177.170 |
|
C2 |
N1 |
H4 |
161.304 |
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 |
-0.568 |
|
|
|
2 |
C |
0.075 |
|
|
|
3 |
S |
0.095 |
|
|
|
4 |
H |
0.398 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.600 |
3.483 |
0.000 |
3.534 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.133 |
1.608 |
0.000 |
y |
1.608 |
-16.903 |
0.000 |
z |
0.000 |
0.000 |
-25.231 |
|
Traceless |
| x | y | z |
x |
-4.066 |
1.608 |
0.000 |
y |
1.608 |
8.280 |
0.000 |
z |
0.000 |
0.000 |
-4.213 |
|
Polar |
3z2-r2 | -8.427 |
x2-y2 | -8.231 |
xy | 1.608 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.977 |
-0.216 |
0.000 |
y |
-0.216 |
8.674 |
0.000 |
z |
0.000 |
0.000 |
1.938 |
<r2> (average value of r
2) Å
2
<r2> |
62.808 |
(<r2>)1/2 |
7.925 |
Jump to
S1C1
Energy calculated at HSEh1PBE/6-31G
| hartrees |
Energy at 0K | -491.334714 |
Energy at 298.15K | |
HF Energy | -491.334714 |
Nuclear repulsion energy | 78.419142 |
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 |
Σ |
3969 |
3796 |
692.41 |
|
|
|
2 |
Σ |
2200 |
2105 |
566.61 |
|
|
|
3 |
Σ |
799 |
764 |
25.21 |
|
|
|
4 |
Π |
440 |
421 |
2.80 |
|
|
|
4 |
Π |
440 |
421 |
2.80 |
|
|
|
5 |
Π |
177i |
170i |
251.07 |
|
|
|
5 |
Π |
177i |
170i |
251.07 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3746.5 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 3583.9 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 C∞v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
N1 |
0.000 |
0.000 |
-1.705 |
C2 |
0.000 |
0.000 |
-0.521 |
S3 |
0.000 |
0.000 |
1.110 |
H4 |
0.000 |
0.000 |
-2.695 |
Atom - Atom Distances (Å)
|
N1 |
C2 |
S3 |
H4 |
N1 | | 1.1842 | 2.8143 | 0.9899 |
C2 | 1.1842 | | 1.6302 | 2.1741 | S3 | 2.8143 | 1.6302 | | 3.8043 | H4 | 0.9899 | 2.1741 | 3.8043 | |
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/6-31G
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
N |
-0.573 |
|
|
|
2 |
C |
0.082 |
|
|
|
3 |
S |
0.088 |
|
|
|
4 |
H |
0.403 |
|
|
|
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 |
-3.698 |
3.698 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.225 |
0.000 |
0.000 |
y |
0.000 |
-25.225 |
0.000 |
z |
0.000 |
0.000 |
-16.363 |
|
Traceless |
| x | y | z |
x |
-4.431 |
0.000 |
0.000 |
y |
0.000 |
-4.431 |
0.000 |
z |
0.000 |
0.000 |
8.861 |
|
Polar |
3z2-r2 | 17.723 |
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 |
1.937 |
0.000 |
0.000 |
y |
0.000 |
1.937 |
0.000 |
z |
0.000 |
0.000 |
8.606 |
<r2> (average value of r
2) Å
2
<r2> |
62.839 |
(<r2>)1/2 |
7.927 |