A Modern Approach to Quantum Mechanics · Problem 6.2

The One-Dimensional Harmonic Oscillator — John S. Townsend

Physics — Quantum Mechanics · position-operator-momentum-space

Problem

Show that ⟨p∣x^∣ψ⟩=iℏ∂∂p⟨p∣ψ⟩\langle p|\hat{x}|\psi\rangle = i\hbar \frac{\partial}{\partial p}\langle p|\psi\rangle and ⟨φ∣x^∣ψ⟩=∫dp ⟨p∣φ⟩∗iℏ∂∂p⟨p∣ψ⟩\langle \varphi|\hat{x}|\psi\rangle = \int dp\, \langle p|\varphi\rangle^* i\hbar \frac{\partial}{\partial p}\langle p|\psi\rangle What do these results suggest for how you should represent the position operator in momentum space?

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