Jump to
S1C2
S2C1
S2C2
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.294682 |
| Energy at 298.15K | -131.293959 |
| HF Energy | -131.294682 |
| Nuclear repulsion energy | 47.488580 |
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 PBE1PBE/6-311G**
| 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' |
3403 |
3265 |
42.41 |
|
|
|
| 2 |
A' |
1804 |
1731 |
39.28 |
|
|
|
| 3 |
A' |
1241 |
1190 |
8.29 |
|
|
|
| 4 |
A' |
467 |
448 |
10.61 |
|
|
|
| 5 |
A' |
348 |
334 |
36.67 |
|
|
|
| 6 |
A" |
454 |
436 |
1.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3858.4 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3701.8 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 PBE1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.058 |
-1.216 |
0.000 |
| C2 |
0.000 |
0.087 |
0.000 |
| N3 |
-0.131 |
1.276 |
0.000 |
| H4 |
0.566 |
-2.157 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3042 | 2.4986 | 1.0695 |
C2 | 1.3042 | | 1.1956 | 2.3147 | N3 | 2.4986 | 1.1956 | | 3.5030 | H4 | 1.0695 | 2.3147 | 3.5030 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.284 |
|
C2 |
C1 |
H4 |
154.268 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.294324 |
| Energy at 298.15K | |
| HF Energy | -131.294324 |
| Nuclear repulsion energy | 47.542544 |
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 PBE1PBE/6-311G**
| 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 |
3456 |
3316 |
70.29 |
|
|
|
| 2 |
Σ |
1744 |
1673 |
42.25 |
|
|
|
| 3 |
Σ |
1277 |
1225 |
5.95 |
|
|
|
| 4 |
Π |
455 |
436 |
0.40 |
|
|
|
| 4 |
Π |
455 |
436 |
0.40 |
|
|
|
| 5 |
Π |
230i |
221i |
48.38 |
|
|
|
| 5 |
Π |
230i |
221i |
48.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3463.3 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3322.7 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 PBE1PBE/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.206 |
| C2 |
0.000 |
0.000 |
0.083 |
| N3 |
0.000 |
0.000 |
1.286 |
| H4 |
0.000 |
0.000 |
-2.271 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2886 | 2.4920 | 1.0652 |
C2 | 1.2886 | | 1.2034 | 2.3538 | N3 | 2.4920 | 1.2034 | | 3.5572 | H4 | 1.0652 | 2.3538 | 3.5572 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.052 |
|
|
|
| 2 |
C |
0.032 |
|
|
|
| 3 |
N |
-0.253 |
|
|
|
| 4 |
H |
0.168 |
|
|
|
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 |
-3.256 |
3.256 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.205 |
0.000 |
0.000 |
| y |
0.000 |
-17.205 |
0.000 |
| z |
0.000 |
0.000 |
-15.364 |
|
| Traceless |
| | x | y | z |
| x |
-0.921 |
0.000 |
0.000 |
| y |
0.000 |
-0.921 |
0.000 |
| z |
0.000 |
0.000 |
1.841 |
|
| Polar |
| 3z2-r2 | 3.682 |
| 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 |
1.914 |
0.000 |
0.000 |
| y |
0.000 |
1.914 |
0.000 |
| z |
0.000 |
0.000 |
6.342 |
<r2> (average value of r
2) Å
2
| <r2> |
35.865 |
| (<r2>)1/2 |
5.989 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.262532 |
| Energy at 298.15K | -131.261996 |
| HF Energy | -131.262532 |
| Nuclear repulsion energy | 47.169229 |
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 PBE1PBE/6-311G**
| 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' |
3089 |
2963 |
5.89 |
|
|
|
| 2 |
A' |
2125 |
2039 |
22.34 |
|
|
|
| 3 |
A' |
1099 |
1054 |
35.24 |
|
|
|
| 4 |
A' |
939 |
901 |
46.99 |
|
|
|
| 5 |
A' |
461 |
442 |
25.18 |
|
|
|
| 6 |
A" |
323 |
310 |
10.67 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4017.8 cm
-1
Scaled (by 0.9594) Zero Point Vibrational Energy (zpe) 3854.7 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 PBE1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.054 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.203 |
1.249 |
0.000 |
| H4 |
1.097 |
-1.629 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3714 | 2.5407 | 1.1003 |
C2 | 1.3714 | | 1.1750 | 2.0403 | N3 | 2.5407 | 1.1750 | | 3.1576 | H4 | 1.1003 | 2.0403 | 3.1576 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.033 |
|
|
|
| 2 |
C |
0.093 |
|
|
|
| 3 |
N |
-0.230 |
|
|
|
| 4 |
H |
0.170 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.770 |
-1.408 |
0.000 |
2.262 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.973 |
-2.535 |
0.000 |
| y |
-2.535 |
-20.937 |
0.000 |
| z |
0.000 |
0.000 |
-15.825 |
|
| Traceless |
| | x | y | z |
| x |
1.408 |
-2.535 |
0.000 |
| y |
-2.535 |
-4.538 |
0.000 |
| z |
0.000 |
0.000 |
3.130 |
|
| Polar |
| 3z2-r2 | 6.260 |
| x2-y2 | 3.964 |
| xy | -2.535 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.584 |
-0.618 |
0.000 |
| y |
-0.618 |
6.322 |
0.000 |
| z |
0.000 |
0.000 |
2.429 |
<r2> (average value of r
2) Å
2
| <r2> |
36.130 |
| (<r2>)1/2 |
6.011 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBE1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.262532 |
| Energy at 298.15K | -131.261996 |
| HF Energy | -131.262532 |
| Nuclear repulsion energy | 47.169229 |
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 PBE1PBE/6-311G**
Geometric Data calculated at PBE1PBE/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability