Jump to
S1C2
S2C1
S2C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -131.294146 |
| Energy at 298.15K | -131.293363 |
| HF Energy | -131.294146 |
| Nuclear repulsion energy | 47.141703 |
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 PBEPBE/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' |
3334 |
3303 |
43.17 |
|
|
|
| 2 |
A' |
1797 |
1780 |
24.91 |
|
|
|
| 3 |
A' |
1222 |
1211 |
4.05 |
|
|
|
| 4 |
A' |
446 |
442 |
7.00 |
|
|
|
| 5 |
A' |
321 |
318 |
45.27 |
|
|
|
| 6 |
A" |
441 |
437 |
1.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3779.9 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 3745.5 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 PBEPBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.058 |
-1.221 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.125 |
1.288 |
0.000 |
| H4 |
0.528 |
-2.189 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3063 | 2.5156 | 1.0754 |
C2 | 1.3063 | | 1.2104 | 2.3329 | N3 | 2.5156 | 1.2104 | | 3.5371 | H4 | 1.0754 | 2.3329 | 3.5371 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.613 |
|
C2 |
C1 |
H4 |
156.653 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -131.293896 |
| Energy at 298.15K | |
| HF Energy | -131.293896 |
| Nuclear repulsion energy | 47.180877 |
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 PBEPBE/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 |
3382 |
3351 |
67.55 |
|
|
|
| 2 |
Σ |
1768 |
1752 |
24.70 |
|
|
|
| 3 |
Σ |
1244 |
1233 |
3.24 |
|
|
|
| 4 |
Π |
442 |
438 |
0.50 |
|
|
|
| 4 |
Π |
442 |
438 |
0.50 |
|
|
|
| 5 |
Π |
215i |
213i |
48.23 |
|
|
|
| 5 |
Π |
215i |
213i |
48.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3423.9 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 3392.7 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 PBEPBE/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.214 |
| C2 |
0.000 |
0.000 |
0.081 |
| N3 |
0.000 |
0.000 |
1.297 |
| H4 |
0.000 |
0.000 |
-2.285 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2952 | 2.5109 | 1.0715 |
C2 | 1.2952 | | 1.2157 | 2.3667 | N3 | 2.5109 | 1.2157 | | 3.5824 | H4 | 1.0715 | 2.3667 | 3.5824 | |
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 PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.040 |
|
|
|
| 2 |
C |
0.016 |
|
|
|
| 3 |
N |
-0.216 |
|
|
|
| 4 |
H |
0.160 |
|
|
|
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 |
-3.163 |
3.163 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.238 |
0.000 |
0.000 |
| y |
0.000 |
-17.238 |
0.000 |
| z |
0.000 |
0.000 |
-15.438 |
|
| Traceless |
| | x | y | z |
| x |
-0.900 |
0.000 |
0.000 |
| y |
0.000 |
-0.900 |
0.000 |
| z |
0.000 |
0.000 |
1.800 |
|
| Polar |
| 3z2-r2 | 3.600 |
| 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 |
1.943 |
0.000 |
0.000 |
| y |
0.000 |
1.943 |
0.000 |
| z |
0.000 |
0.000 |
6.533 |
<r2> (average value of r
2) Å
2
| <r2> |
36.271 |
| (<r2>)1/2 |
6.023 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -131.267393 |
| Energy at 298.15K | -131.266815 |
| HF Energy | -131.267393 |
| Nuclear repulsion energy | 46.774414 |
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 PBEPBE/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' |
2993 |
2965 |
8.56 |
|
|
|
| 2 |
A' |
2019 |
2001 |
16.13 |
|
|
|
| 3 |
A' |
1091 |
1081 |
19.52 |
|
|
|
| 4 |
A' |
893 |
885 |
62.46 |
|
|
|
| 5 |
A' |
451 |
447 |
22.09 |
|
|
|
| 6 |
A" |
305 |
302 |
8.46 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3875.1 cm
-1
Scaled (by 0.9909) Zero Point Vibrational Energy (zpe) 3839.9 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 PBEPBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.242 |
-1.259 |
0.000 |
| C2 |
0.000 |
0.089 |
0.000 |
| N3 |
-0.397 |
1.216 |
0.000 |
| H4 |
1.327 |
-1.486 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3698 | 2.5558 | 1.1086 |
C2 | 1.3698 | | 1.1943 | 2.0596 | N3 | 2.5558 | 1.1943 | | 3.2047 | H4 | 1.1086 | 2.0596 | 3.2047 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.057 |
|
|
|
| 2 |
C |
0.083 |
|
|
|
| 3 |
N |
-0.193 |
|
|
|
| 4 |
H |
0.167 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.858 |
-1.068 |
0.000 |
2.143 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.472 |
-1.795 |
0.000 |
| y |
-1.795 |
-21.337 |
0.000 |
| z |
0.000 |
0.000 |
-15.846 |
|
| Traceless |
| | x | y | z |
| x |
2.119 |
-1.795 |
0.000 |
| y |
-1.795 |
-5.177 |
0.000 |
| z |
0.000 |
0.000 |
3.058 |
|
| Polar |
| 3z2-r2 | 6.116 |
| x2-y2 | 4.865 |
| xy | -1.795 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.940 |
-1.187 |
0.000 |
| y |
-1.187 |
6.300 |
0.000 |
| z |
0.000 |
0.000 |
2.405 |
<r2> (average value of r
2) Å
2
| <r2> |
36.497 |
| (<r2>)1/2 |
6.041 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBEPBE/6-311G**
| | hartrees |
| Energy at 0K | -131.267393 |
| Energy at 298.15K | -131.266815 |
| HF Energy | -131.267393 |
| Nuclear repulsion energy | 46.774414 |
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 PBEPBE/6-311G**
Geometric Data calculated at PBEPBE/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability