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Consider a particle with mass m described by the Hamilton operator for a one-dimensional harmonic oscillator 2 Zm 2 The normalized eigenfunctions for Hare φη (x) with energies E,,-(n + 2) ha. At time t-0 the wavefunction of the particle is given by у(x,0)- (V3іфі (x) + ф3(x)). Now let H be an operator given by where k is a positive constant. 1) Show that H is Hermitian. 2) Express H by the step-operators a+ and a 3) Calculate the expectation value of H in the state ψ(x,0).

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