Chapter 4

The problems in this chapter are focused on density operators.

Background material

The most frequent use of density operators/matrices is describing the statistical state of a quantum systems. In other words given all possible pure states whats the probability of any given state.

The expectation of a hermitian matrix corresponding to an observable corresponds to the average given by:

O^tr(O^ρ) \langle \hat{O} \rangle \coloneqq \text{tr}(\hat{O} \rho)

where ρ\rho is the density matrix that can describe a pure or mixed state. In the case of a pure state its simply given by ρ=ψψ\rho=\ket{\psi}\bra{\psi} and has the property that ρ2=ρ\rho^2 = \rho , i.e., idempotent.

Problems

Programing Problems