Jump to
S1C2
S1C3
Energy calculated at B2PLYP=FULL/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.667400 |
| Energy at 298.15K | -692.666787 |
| HF Energy | -692.430593 |
| Nuclear repulsion energy | 60.966832 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B2PLYP=FULL/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.309 |
| C2 |
0.000 |
0.000 |
-1.284 |
| N3 |
0.000 |
0.000 |
-2.454 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.5928 | 3.7628 |
C2 | 2.5928 | | 1.1700 | N3 | 3.7628 | 1.1700 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
180.000 |
|
K1 |
N3 |
C2 |
0.000 |
| C2 |
K1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C3
Energy calculated at B2PLYP=FULL/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.669641 |
| Energy at 298.15K | |
| HF Energy | -692.435476 |
| Nuclear repulsion energy | 64.423311 |
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 B2PLYP=FULL/6-311+G(3df,2p)
| 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 |
2085 |
2085 |
98.84 |
|
|
|
| 2 |
Σ |
311 |
311 |
84.07 |
|
|
|
| 3 |
Π |
35i |
35i |
1.14 |
|
|
|
| 3 |
Π |
36i |
36i |
1.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1162.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 1162.5 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 B2PLYP=FULL/6-311+G(3df,2p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
0.000 |
1.211 |
| C2 |
0.000 |
0.000 |
-2.404 |
| N3 |
0.000 |
0.000 |
-1.227 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 3.6159 | 2.4388 |
C2 | 3.6159 | | 1.1771 | N3 | 2.4388 | 1.1771 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
0.000 |
|
K1 |
N3 |
C2 |
180.000 |
| C2 |
K1 |
N3 |
0.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at B2PLYP=FULL/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -692.673205 |
| Energy at 298.15K | -692.673052 |
| HF Energy | -692.437498 |
| Nuclear repulsion energy | 68.486949 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Geometric Data calculated at B2PLYP=FULL/6-311+G(3df,2p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| K1 |
0.000 |
1.046 |
0.000 |
| C2 |
0.626 |
-1.630 |
0.000 |
| N3 |
-0.536 |
-1.442 |
0.000 |
Atom - Atom Distances (Å)
| |
K1 |
C2 |
N3 |
| K1 | | 2.7484 | 2.5447 |
C2 | 2.7484 | | 1.1772 | N3 | 2.5447 | 1.1772 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| K1 |
C2 |
N3 |
67.616 |
|
K1 |
N3 |
C2 |
87.058 |
| C2 |
K1 |
N3 |
25.326 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability