Chapter 8

The problems of this chapter are focused on measurement probability.

Background material

In quantum theory the mathematics that describes the observation of a physical occuring event (process) is only provided probabilistically. This means that the physical system in the quantum state Φ|\Phi\rangle can actually be discussed as having a probability of being in a quantum state Ψ|\Psi\rangle, this is given as:

ΦΨ2. \left| \langle \Phi | \Psi \rangle \right|^2 .

If Φ=Ψ|\Phi\rangle = |\Psi\rangle, then its the probability of being is a specific quantum state Ψ|\Psi\rangle. The outcome for a measurement, more specifically a measurement operator corresponding to an observable in some state ψ\psi, has a probability:

pi=ψOiOiψ p_i = \langle \psi | \mathcal{O}^{\dagger}_i \mathcal{O}_i | \psi \rangle

where ii corresponds to a specific measurment outcome, for example, spin-up or spin-down of an electron. Because something had to happen during the outcome of applying a measurment operator or equally saying "observing a measurement", the set of outcomes – our spin-up and spin-down for example – requires that they form a complete set. This is represented by the completeness equation:

iOiOi=I, \sum_i \mathcal{O}^{\dagger}_i \mathcal{O}_i = \mathbf{I},

where I\mathbf{I} is the identity. In the example of spin-up and spin-down particles the two operators in matrix form are:

P=(1000)P=(0001) P_{\uparrow} = \begin{pmatrix} 1 & 0 \\ 0 & 0 \end{pmatrix} \hskip{3mm} P_{\downarrow} = \begin{pmatrix} 0 & 0 \\ 0 & 1 \end{pmatrix}

Problems

Programing Problems