
Chapter 5
Mixed States, Open Systems, and
the Density Operator
The formalism for quantum systems developed so far applies to what are
called pure states. A system in a pure state is completely specified by the
state vector. A complete set of experimental tests will determine the system
state fully: we have maximal knowledge of the system. For example, for a spin
system, we can find a particular orientation of an SG machine such that the
state is in its + or − port. This also means that the state is an eigenvector of
some operator, or is always a linear combination of the computational basis
states.
As opposed to this, as in most practical cases, we only ...