Franz Schwabl Quantum Mechanics 4th Edit · Problem 9.3

Addition of Angular Momenta

Physics — Quantum Mechanics · spin-eigenstates-rotation

Problem

Show that the states ∣e,±⟩=e−iαSy/ℏ{∣↑⟩∣↓⟩|\boldsymbol{e}, \pm\rangle = \mathrm{e}^{-\mathrm{i}\alpha S_y/\hbar}\begin{cases}|{\uparrow}\rangle \\ |{\downarrow}\rangle\end{cases} are eigenstates of the projection of the spin operator in the direction of e=(sin⁡α,0,cos⁡α)  .\boldsymbol{e} = (\sin\alpha, 0, \cos\alpha) \;. Hint: Compute S′=e−iαSy/ℏ S eiαSy/ℏ\boldsymbol{S}' = \mathrm{e}^{-\mathrm{i}\alpha S_y/\hbar}\, \boldsymbol{S}\, \mathrm{e}^{\mathrm{i}\alpha S_y/\hbar} and show that Sz′=S⋅eS'_z = \boldsymbol{S} \cdot \boldsymbol{e}.

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