Non-Crossing Rule for Energy Curves in Diatomic Molecules
Non-Crossing Rule for Energy Curves in Diatomic Molecules
Let (R) and (R) be energy curves for two different electronic states of a diatomic molecule, both computed within the Born–Oppenheimer approximation. If the two states belong to different symmetry species, say and , and , or singlet and triplet, there is no restriction on whether the curves can cross. If, however, the two states have the same symmetry, a non-crossing rule applies. Close approach of the two curves results in mutual repulsion, known as an anticrossing. For near degeneracy of (R) and (R), a perturbation (R), representing higher-order contributions in the Born–Oppenheimer approximation, becomes significant, giving mixed states that do not cross.
E
1
E
2
Σ
Π
u
g
E
1
E
2
V
12
In this Demonstration, the lower energy state, (R), is drawn in blue. It is assumed to be a bonding state, with dissociation energy and equilibrium internuclear distance , which can both be varied with sliders. The upper energy state, (R), drawn in red, is assumed to be a repulsive state. The mixing parameter can also be varied. In certain cases, the upper state can develop a minimum as a result of the interaction. The dashed curves in the graphic pertain when (R)=0.
E
1
D
e
R
e
E
2
V
12
V
12
V
12