Principles of Quantum Mechanics · Problem 7.4.7

The Path Integral Formulation of Quantum Theory — R. Shankar

Physics — Quantum Mechanics · commutator-poisson-bracket-correspondence

Problem

Verify Eq. (7.4.40) for the case (1) Ω=X\Omega = X, Λ=X2+P2\Lambda = X^2 + P^2 (2) Ω=X2\Omega = X^2, Λ=P2\Lambda = P^2 The second case illustrates the ordering ambiguity.
Intuitive explanation

The commutator [Ω,Λ][\Omega, \Lambda] measures whether two quantum operators are compatible—and when it's nonzero, you'll discover that the order in which you write products of XX and PP matters crucially. For case (1), use the canonical commutation relation [X,P]=iℏ[X,P] = i\hbar to expand [Ω,Λ][\Omega, \Lambda] systematically and verify the claimed result. Case (2) reveals the subtlety: X2P2X^2 P^2 can be reordered in multiple ways, and different choices yield different commutators, showing why quantum mechanics requires careful operator algebra—there's no single "right" answer until you specify the ordering convention.

Intuitive explanation

The commutator [Ω,Λ][\Omega, \Lambda] measures whether two quantum operators are compatible—and when it's nonzero, you'll discover that the order in which you write products of XX and PP matters crucially. For case (1), use the canonical commutation relation [X,P]=iℏ[X,P] = i\hbar to expand [Ω,Λ][\Omega, \Lambda] systematically and verify the claimed result. Case (2) reveals the subtlety: X2P2X^2 P^2 can be reordered in multiple ways, and different choices yield different commutators, showing why quantum mechanics requires careful operator algebra—there's no single "right" answer until you specify the ordering convention.

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