Recall that T(a)−1φ(x)T(a)=φ(x−a), where T(a)≡exp(−iPμaμ) is the spacetime translation operator, and P0 is identified as the hamiltonian H.
a) Let aμ be infinitesimal, and derive an expression for [φ(x),Pμ].
b) Show that the time component of your result is equivalent to the Heisenberg equation of motion iφ˙=[φ,H].
c) For a free field, use the Heisenberg equation to derive the Klein-Gordon equation.
d) Define a spatial momentum operator
P≡−∫d3xΠ(x)∇φ(x).(3.36)
Use the canonical commutation relations to show that P obeys the relation you derived in part (a).
e) Express P in terms of a(k) and a†(k).