 Solution

ID: past-exam-of-the-options-i-course-of-the-university-of-oxford/2004/j/j1/i/solution

i ℏ \frac{\partial ψ}{\partial t} = - \frac{ℏ ^{2}}{2 m} Δ ψ + V ψ .

A normalized quantum state has

\int_{R^{3}} ∣ ψ ∣^{2} d^{3} x = 1

; the Hamiltonian operator acts on wave functions satisfying the appropriate domain and boundary conditions.

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