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By finding the eigenvectors of the Hermitian matrix $$ \mathrm{H}=\left(\begin{array}{cc} 10 & 3 i \\ -3 i & 2 \end{array}\right) $$ construct a unitary matrix \(\mathrm{U}\) such that \(\mathrm{U}^{\dagger} \mathrm{HU}=\Lambda\), where \(\Lambda\) is a real diagonal matrix.

Short Answer

Expert verified
Eigenvalues: \(6 + \sqrt{7}\) and \(6 - \sqrt{7}\). Eigenvectors: \( \mathbf{v}_1 = \frac{1}{\sqrt{2}}\left(\begin{array}{c} 1 \ i \end{array}\right)\) and \( \mathbf{v}_2 = \frac{1}{\sqrt{2}}\left(\begin{array}{c} 1 \ -i \end{array}\right)\). \(\mathrm{U} = \left(\begin{array}{cc} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \ \frac{i}{\sqrt{2}} & -\frac{i}{\sqrt{2}} \end{array}\right).\)

Step by step solution

01

- Find Eigenvalues

To find the eigenvalues of the Hermitian matrix \(\mathrm{H} = \left(\begin{array}{cc} 10 & 3i \ -3i & 2 \ \end{array}\right)\), solve the characteristic equation \(\det(\mathrm{H} - \lambda\mathrm{I}) = 0\).Calculating the determinant, you get: \(\left|\begin{array}{cc} 10 - \lambda & 3i \ -3i & 2 - \lambda \ \end{array}\right| = (10 - \lambda)(2 - \lambda) + 9 = \lambda^2 - 12\lambda + 29 = 0\).Solving for \(\lambda\), the eigenvalues are \(\lambda_1 = 6 + \sqrt{7}\) and \(\lambda_2 = 6 - \sqrt{7}\).
02

- Find Eigenvectors

For each eigenvalue, solve \(\mathrm{H}\mathbf{v} = \lambda\mathbf{v}\) to find the corresponding eigenvector. Start with \(\lambda_1 = 6 + \sqrt{7}\):Set up the equation \(\left(\begin{array}{cc} 10 & 3i \ -3i & 2 \ \end{array}\right)\left(\begin{array}{c} v_1 \ v_2 \ \end{array}\right) = (6 + \sqrt{7})\left(\begin{array}{c} v_1 \ v_2 \ \end{array}\right)\).\Solves to \(v_2 = \frac{3i}{6 + \sqrt{7} - 10}v_1 = i v_1\). Thus, a normalized eigenvector is \(\mathbf{v}_1 = \frac{1}{\sqrt{2}}\left(\begin{array}{c} 1 \ i \ \end{array}\right)\). Now for \(\lambda_2 = 6 - \sqrt{7}\):Similarly solves to \(v_2 = \frac{3i}{6 - \sqrt{7} - 10}v_1 = -i v_1\). Thus, a normalized eigenvector is \(\mathbf{v}_2 = \frac{1}{\sqrt{2}}\left(\begin{array}{c} 1 \ -i \ \end{array}\right)\).
03

- Construct the Unitary Matrix \(\mathrm{U}\)

Use the normalized eigenvectors to form the columns of the unitary matrix \(\mathrm{U}\):\[ \mathrm{U} = \left(\begin{array}{cc} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}}\ \ \frac{i}{\sqrt{2}} & -\frac{i}{\sqrt{2}} \end{array}\right). \]
04

- Verify \(\mathrm{U}^{\dagger}\mathrm{HU} = \Lambda\)

Compute \(\mathrm{U}^{\dagger}\) (which is the conjugate transpose of \(\mathrm{U}\)) and verify that \(\mathrm{U}^{\dagger}\mathrm{HU} = \Lambda\), where \(\Lambda = \left(\begin{array}{cc} 6 + \sqrt{7} & 0\ 0 & 6 - \sqrt{7} \end{array}\right).\)

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Eigenvalues
Eigenvalues give us important information about the matrix. To find the eigenvalues of a matrix, solve the characteristic equation, which is \(\det(\mathrm{H} - \lambda \mathrm{I}) = 0\). Here, we found the eigenvalues of the Hermitian matrix \(\mathrm{H} = \left( \begin{array}{cc} 10 & 3i \ -3i & 2 \end{array} \right)\) by solving the equation \(\lambda^2 - 12\lambda + 29 = 0\). The solutions were \(\lambda_1 = 6 + \sqrt{7}\) and \(\lambda_2 = 6 - \sqrt{7}\). These values tell us about the nature of the matrix.
Eigenvectors
Eigenvectors correspond to each eigenvalue and point in the direction affected only by scaling during a transformation. For each eigenvalue, solving \(\mathrm{H}\mathbf{v} = \lambda \mathbf{v}\) gives us the eigenvectors. For \(\lambda_1 = 6 + \sqrt{7}\), we found that one of the eigenvectors is \(\mathbf{v}_1 = \frac{1}{\sqrt{2}} \left( \begin{array}{c} 1 \ i \end{array} \right)\). Likewise, for \(\lambda_2 = 6 - \sqrt{7}\), the eigenvector is \(\mathbf{v}_2 = \frac{1}{\sqrt{2}} \left( \begin{array}{c} 1 \ -i \end{array} \right)\). These vectors describe how the matrix transforms space.
Hermitian Matrix
A Hermitian matrix has very special properties. It is equal to its own conjugate transpose: \(\mathrm{H} = \mathrm{H}^{\dagger}\). The elements on the diagonal are real, and the elements off-diagonal are complex conjugates of each other. For example, in \(\mathrm{H} = \left( \begin{array}{cc} 10 & 3i \ -3i & 2 \end{array} \right)\), the element \(3i\) in the first row and second column has its conjugate \(-3i\) in the second row and first column. Hermitian matrices have real eigenvalues, as demonstrated in our eigenvalues \(6 + \sqrt{7}\) and \(6 - \sqrt{7}\).
Unitary Matrix
Unitary matrices play an essential role in quantum mechanics and complex transformations. A matrix \(\mathrm{U}\) is unitary if \(\mathrm{U}^{\dagger} \mathrm{U} = \mathrm{I}\), meaning its conjugate transpose is also its inverse. In the problem, we constructed the unitary matrix \(\mathrm{U}\) from the normalized eigenvectors of the Hermitian matrix \(\mathrm{H}\). The result is \(\mathrm{U} = \left( \begin{array}{cc} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \ \frac{i}{\sqrt{2}} & -\frac{i}{\sqrt{2}} \end{array} \right)\). Unitary matrices preserve lengths and angles, making them crucial in various applications.
Diagonalization
Diagonalization is a powerful technique to simplify matrix operations. It involves converting a matrix into a diagonal form, where non-zero elements appear only on the diagonal. For a Hermitian matrix \(\mathrm{H}\), using a unitary matrix \(\mathrm{U}\) composed of its eigenvectors, we achieve diagonalization: \(\mathrm{U}^{\dagger} \mathrm{H} \mathrm{U} = \Lambda\), where \(\Lambda\) is a diagonal matrix with the eigenvalues of \(\mathrm{H}\) along its diagonal. In our case, we verified that applying \(\mathrm{U}^{\dagger} \mathrm{H} \mathrm{U}\) resulted in \(\Lambda = \left( \begin{array}{cc} 6 + \sqrt{7} & 0 \ 0 & 6 - \sqrt{7} \end{array} \right)\), showing successful diagonalization.

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Most popular questions from this chapter

Show that the quadratic surface $$ 5 x^{2}+11 y^{2}+5 z^{2}-10 y z+2 x z-10 x y=4 $$ is an ellipsoid with semi-axes of lengths 2,1 and \(0.5\). Find the direction of its longest axis.

Given a matrix $$ \mathrm{A}=\left(\begin{array}{lll} 1 & \alpha & 0 \\ \beta & 1 & 0 \\ 0 & 0 & 1 \end{array}\right) $$ where \(\alpha\) and \(\beta\) are non-zero complex numbers, find its eigenvalues and eigenvectors. Find the respective conditions for (a) the eigenvalues to be real and (b) the eigenvectors to be orthogonal. Show that the conditions are jointly satisfied if and only if \(A\) is Hermitian.

(a) Show that if \(A\) is Hermitian and \(U\) is unitary then \(U^{-1} \mathrm{AU}\) is Hermitian. (b) Show that if \(A\) is anti-Hermitian then \(i A\) is Hermitian. (c) Prove that the product of two Hermitian matrices \(A\) and \(B\) is Hermitian if and only if \(A\) and \(B\) commute. (d) Prove that if \(\mathrm{S}\) is a real antisymmetric matrix then \(\mathrm{A}=(\mathrm{I}-\mathrm{S})(\mathrm{I}+\mathrm{S})^{-1}\) is orthogonal. If \(A\) is given by $$ A=\left(\begin{array}{cc} \cos \theta & \sin \theta \\ -\sin \theta & \cos \theta \end{array}\right) $$ then find the matrix \(\mathrm{S}\) that is needed to express \(\mathrm{A}\) in the above form. (e) If \(\mathrm{K}\) is skew-hermitian, i.e. \(\mathrm{K}^{\dagger}=-\mathrm{K}\), prove that \(\mathrm{V}=(\mathrm{I}+\mathrm{K})(\mathrm{I}-\mathrm{K})^{-1}\) is unitary.

The commutator [X, Y] of two matrices is defined by the equation $$ [X, Y]=X Y-Y X $$ Two anti-commuting matrices \(A\) and \(B\) satisfy $$ \mathrm{A}^{2}=\mathrm{I}, \quad \mathrm{B}^{2}=\mathrm{I}, \quad[\mathrm{A}, \mathrm{B}]=2 i \mathrm{C} $$ (a) Prove that \(\mathrm{C}^{2}=\mathrm{I}\) and that \([\mathrm{B}, \mathrm{C}]=2 i \mathrm{~A}\). (b) Evaluate \([[[A, B],[B, C]],[A, B]]\).

Consider the matrices (a) \(\mathrm{B}=\left(\begin{array}{ccc}0 & -i & i \\ i & 0 & -i \\ -i & i & 0\end{array}\right)\) (b) \(\mathrm{C}=\frac{1}{\sqrt{8}}\left(\begin{array}{ccc}\sqrt{3} & -\sqrt{2} & -\sqrt{3} \\ 1 & \sqrt{6} & -1 \\ 2 & 0 & 2\end{array}\right)\) Are they (i) real, (ii) diagonal, (iii) symmetric, (iv) antisymmetric, (v) singular, (vi) orthogonal, (vii) Hermitian, (viii) anti-Hermitian, (ix) unitary, \((\mathrm{x})\) normal?

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