A spin-half particle is in the pure state whose Bloch vector is .

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Symmetry, angular momentum and spin · Symmetry, angular momentum and spin

The Structure of Quantum Mechanics, Ch Spin one-half, SU(2) and two-level dynamics

Problem

A spin-half particle is in the pure state whose Bloch vector is n^=(0, 3/2, −12)\hat n=\bigl(0,\ \sqrt3/2,\ -\tfrac12\bigr). ((a)) Write the state as cos⁡(θ/2)∣↑⟩+eiϕsin⁡(θ/2)∣↓⟩\cos(\theta/2)|\uparrow\rangle+e^{i\phi}\sin(\theta/2)|\downarrow\rangle, giving θ\theta, ϕ\phi and the two coefficients. ((b)) Find the probability that a measurement of spin along m^=(x^+z^)/2\hat m=(\hat x+\hat z)/\sqrt2 gives +ℏ/2+\hbar/2.

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