Someone works through the translation operator as follows."Since for every position…

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · The formalism of quantum mechanics · The formalism of quantum mechanics

The Structure of Quantum Mechanics, Ch Position, momentum and the origin of the canonical commutator

Problem

Someone works through the translation operator as follows."Since T^(a)∣x⟩=∣x+a⟩\hat T(a)|x\rangle = |x+a\rangle for every position eigenvector, and ∣ψ⟩=∫dx ψ(x)∣x⟩|\psi\rangle = \int dx\,\psi(x)|x\rangle, it follows that T^(a)∣ψ⟩=∫dx ψ(x) T^(a)∣x⟩=∫dx ψ(x)∣x+a⟩.\hat T(a)|\psi\rangle = \int dx\,\psi(x)\,\hat T(a)|x\rangle = \int dx\,\psi(x)|x+a\rangle. Relabelling the dummy integration variable as x′=x+ax' = x+a, so that x=x′−ax = x'-a, this is T^(a)∣ψ⟩=∫dx′ ψ(x′−a)∣x′⟩,\hat T(a)|\psi\rangle = \int dx'\,\psi(x'-a)|x'\rangle, so the new wave function seen at the point labelled x′x' is ⟨x′∣T^(a)∣ψ⟩=ψ(x′−a)\langle x'|\hat T(a)|\psi\rangle = \psi(x'-a). But since T^(a)\hat T(a) shifts every basis label xx up by aa, the wave function itself must shift up by aa too, so the final answer is ⟨x∣T^(a)∣ψ⟩=ψ(x+a).\langle x|\hat T(a)|\psi\rangle = \psi(x+a)." ((a)) Find the step where the error occurs. ((b)) State the correct relation between ⟨x∣T^(a)∣ψ⟩\langle x|\hat T(a)|\psi\rangle and ψ\psi, and explain in one sentence why a positive aa moves the graph of the wave function to the right rather than shifting its formula by +a+a.

Related theory

Browse the problem library