, where
- is the Hamiltonian
- is the eigenvalue, also known as the Energy of the Eigenstate.
The time-independent Schrodinger Equation is easier to solve, and it provides the Eigenstates needed to describe the general solution.
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H∣ψ⟩=E∣ψ⟩, where
The time-independent Schrodinger Equation is easier to solve, and it provides the Eigenstates needed to describe the general solution.