SUMMARY
The discussion centers on whether a wave function that is a linear combination of two energy eigenstates satisfies the time-independent Schrödinger equation (TISE). It is established that energy eigenstates satisfy the eigenvalue equation defined by the Hamiltonian operator, expressed as H|E⟩ = E|E⟩. A linear combination of two eigenstates, |ψ⟩ = c₁|E₁⟩ + c₂|E₂⟩, does not generally satisfy the TISE unless the coefficients correspond to degenerate states, where both eigenstates have the same energy. The key takeaway is that for |ψ⟩ to satisfy the TISE, it must be expressible as H|ψ⟩ = E|ψ⟩ for some constant E.
PREREQUISITES
- Understanding of the Hamiltonian operator in quantum mechanics
- Familiarity with energy eigenstates and eigenvalue equations
- Knowledge of linear combinations of quantum states
- Basic grasp of the time-independent Schrödinger equation
NEXT STEPS
- Study the properties of the Hamiltonian operator in quantum mechanics
- Learn about eigenstates and eigenvalues in quantum systems
- Explore the implications of linear combinations of quantum states
- Investigate conditions under which linear combinations can be eigenstates
USEFUL FOR
Students and professionals in quantum mechanics, physicists exploring wave functions, and anyone studying the mathematical foundations of quantum theory.