Measurements are described by sets of measurement operators {Aim}, where the index m corresponds to any of the possible outcomes of the measurement. Measurement of a single qubit in the computational basis is described by the operators Outcome 0 : Mb 2 lUXUI Outcome 1 : M] = l1)(1| . Suppose a qubit is in the normalized state is?) from part (a). What are the probabilities of outcomes 0 and 1 when is?) is measured in the computational basis