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Quantum Mechanics : Given a Matrix (Hamiltonian) of the form ſa b a) Find the Eigenvalues b) Find the Eigenvectors c) Use the

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Answer #1

To find the eigenvalues you need to compute, \text{det}(H - \lambda \matcal{I}_2) = 0. I_2 is the indentity matrix of dimension 2. So on solving this we get an algebric equation (quadratic equation) in \lambda , a d-a \lambda -b^2-d \lambda +\lambda ^2 = 0. Now solving for \lambda we get, \lambda_{1, 2} = \frac{1}{2} \left(-\sqrt{(a-d)^2+4 b^2}+a+d\right),\frac{1}{2} \left(\sqrt{(a-d)^2+4 b^2}+a+d\right).

Now to compute the eigenvectors one needs to plug in 1.29 into H - \lambda_{1, 2} I_2 = (x_1, x_2)^{T}. Solving for x_1, x_2 will lead to pair of linear equations which on solving will lead to two different pairs of values of x_1, x_2 which leads to the eigenvectors. They are, x_1, x_2 = \left\{-\frac{\sqrt{a^2-2 a d+4 b^2+d^2}-a+d}{2 b},1\right\}^{T},\left\{-\frac{-\sqrt{a^2-2 a d+4 b^2+d^2}-a+d}{2 b},1\right\}^{T}.

Now, for the spin polarisation part, S_{\pm} = \left\{\frac{\left(\sqrt{a^2-2 a d+4 b^2+d^2}-a+d\right)^2}{4 b^2}-\frac{\left(-\sqrt{a^2-2 a d+4 b^2+d^2}-a+d\right)^2}{4 b^2},0\right\}^{T}.

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