Srednicki — Quantum Field Theory · Problem 3.4

Canonical Quantization of Scalar Fields — Mark Srednicki

Physics — QFT · canonical-quantization-scalar-fields

Problem

Recall that T(a)−1φ(x)T(a)=φ(x−a)T(a)^{-1}\varphi(x)T(a) = \varphi(x-a), where T(a)≡exp⁡(−iPμaμ)T(a) \equiv \exp(-iP^\mu a_\mu) is the spacetime translation operator, and P0P^0 is identified as the hamiltonian HH. a) Let aμa^\mu be infinitesimal, and derive an expression for [φ(x),Pμ][\varphi(x), P^\mu]. b) Show that the time component of your result is equivalent to the Heisenberg equation of motion iφ˙=[φ,H]i\dot{\varphi} = [\varphi, H]. c) For a free field, use the Heisenberg equation to derive the Klein-Gordon equation. d) Define a spatial momentum operator P≡−∫d3x Π(x)∇φ(x) .(3.36)\mathbf{P} \equiv -\int d^3x\,\Pi(x)\nabla\varphi(x)\,. \tag{3.36} Use the canonical commutation relations to show that P\mathbf{P} obeys the relation you derived in part (a). e) Express P\mathbf{P} in terms of a(k)a(\mathbf{k}) and a†(k)a^\dagger(\mathbf{k}).

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