Principles of Quantum Mechanics · Problem 14.3.1

Spin — R. Shankar

Physics — Quantum Mechanics · spin-spinor-eigenket

Problem

Let us verify the above corollary explicitly. Take some spinor with components α=ρ1eiϕ1\alpha = \rho_1 e^{i\phi_1} and β=ρ2eiϕ2\beta = \rho_2 e^{i\phi_2}. From ⟨χ∣χ⟩=1\langle \chi | \chi \rangle = 1, deduce that we can write ρ1=cos⁡(θ/2)\rho_1 = \cos(\theta/2) and ρ2=sin⁡(θ/2)\rho_2 = \sin(\theta/2) for some θ\theta. Next pull out a common phase factor so that the spinor takes the form in Eq. (14.3.28a). This verifies the corollary and also fixes n^\hat{n}.

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