Excitons in a conjugated polymer can be approximated using it by adding a term for Coulombic force and applying the linear combination of atomic orbitals across the length of the polymer. An n-dimensional version of it will have energy levels of n degeneracy, and if the constraints of this system allow, tunneling can be also be solved for. The Hamiltonian for it is simplified because the potential energy term can be omitted, which allows the set of eigenvalues to be solved exactly, making it useful for modeling more complex systems and as a teaching tool. The wave function is sinusoidal in, for 10 points, what hypothetical construct in quantum mechanics, in which the title entity is confined to a limited space.
Excitons in a conjugated polymer can be approximated using it by adding a term for Coulombic force and applying the linear combination of atomic orbitals across the length of the polymer. An n-dimensional version of it will have energy levels of n degeneracy, and if the constraints of this system allow, tunneling can be also be solved for. The Hamiltonian for it is simplified because the potential energy term can be omitted, which allows the set of eigenvalues to be solved exactly, making it useful for modeling more complex systems and as a teaching tool. The wave function is sinusoidal in, for 10 points, what hypothetical construct in quantum mechanics, in which the title entity is confined to a limited space.
Excitons in a conjugated polymer can be approximated using it by adding a term for Coulombic force and applying the linear combination of atomic orbitals across the length of the polymer.
{Particle} in a {box} [accept {particle} in an {infinite potential well} or {particle} in an {infinite square well}]