Let us verify the above corollary explicitly. Take some spinor with components α=ρ1eiϕ1 and β=ρ2eiϕ2. From ⟨χ∣χ⟩=1, deduce that we can write ρ1=cos(θ/2) and ρ2=sin(θ/2) for some θ. 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^.