Principles of Quantum Mechanics · Problem 1.8.3

Mathematical Introduction — R. Shankar

Physics — Quantum Mechanics · eigenvalue-problem-hermitian

Problem

Consider the Hermitian matrix Ω=12[20003−10−13]\Omega = \frac{1}{2}\begin{bmatrix} 2 & 0 & 0 \\ 0 & 3 & -1 \\ 0 & -1 & 3 \end{bmatrix} (1) Show that ω1=ω2=1\omega_1 = \omega_2 = 1; ω3=2\omega_3 = 2. (2) Show that ∣ω=2⟩|\omega = 2\rangle is any vector of the form 1(2a2)1/2[0a−a]\frac{1}{(2a^2)^{1/2}}\begin{bmatrix} 0 \\ a \\ -a \end{bmatrix} (3) Show that the ω=1\omega = 1 eigenspace contains all vectors of the form 1(b2+2c2)1/2[bcc]\frac{1}{(b^2 + 2c^2)^{1/2}}\begin{bmatrix} b \\ c \\ c \end{bmatrix} either by feeding ω=1\omega = 1 into the equations or by requiring that the ω=1\omega = 1 eigenspace be orthogonal to ∣ω=2⟩|\omega = 2\rangle.

Related theory

Browse the problem library