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Introduction to Quantum Mechanics, Spring 2015 Problem Set 12 Due Tuesday, March 24 Problem 1: Consider the Pauli-Schrödinger equation in three space dimensions discussed in class. • Find all the solutions to this equation, and show how the momentum operator and space-translations act on solutions. • Show explicitly how the double-cover of the Euclidean group acts on the space of solutions. • Find a solution of the equation that is a helicity eigenvector (eigenvector of J · P) as well as a momentum eigenvector with momentum only in the z direction. What happens to this solution when you act on it by the double cover of the rotations about the x-axis? Find all the other solutions one gets by acting on this by the double-cover of the Euclidean group. Problem 2: Compute the propagator G(x0 , t0 , x, t) = h0|ψ̂(x0 , t0 )ψ̂ † (x, t)|0i for the free non-relativistic particle of mass m (for t0 > t). First do this in momentum space, showing that 2 k (t0 −t) e 0 , t0 , k, t) = e−i 2m G(k δ(k 0 − k) then Fourier transform to find the position space result G(x0 , t0 , x, t) = ( m 1 − m (x0 −x)2 ) 2 e i2(t0 −t) 0 i2π(t − t) Show also that lim G(x0 , t0 , x, t) = δ(x0 − x) t→t0 Problem 3: Show that if one takes the quantum field theory Hamiltonian operator to be ∞ 1 d2 b ψb† (x)(− + V (x))ψ(x)dx 2m dx2 −∞ Z b = H the field operators will satisfy the conventional Schrödinger equation for the case of a potential V (x). 1 Problem 4: A quantum system corresponding to indistinguishable particles interacting with each other with an interaction energy v(x − y) (where x, y are the positions of the particles) is given by adding a term Z Z 1 ∞ ∞ b† b ψ(x)dxdy b ψ (x)ψb† (y)v(y − x)ψ(y) 2 −∞ −∞ to the free particle Hamiltonian. Just as the free-particle Hamiltonian has an expression as a momentum space integral involving products of annihilation and creation operators, can you write this interaction term as a momentum space integral involving products of annihilation and creation operators (in terms of the Fourier transform of v(x − y)? 2