Regarding Diagonalization of Matrix by Spectral Theorem

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The discussion centers on the diagonalization of a symmetric matrix A using the spectral theorem for self-adjoint operators. The matrix A is structured as follows: A = [ U 0 U; 0 0 0; U 0 U], where U is a square matrix. It is confirmed that the columns of the orthogonal matrix P are indeed the eigenvectors of A, and the transformation applied demonstrates that diagonalization can be achieved by first diagonalizing the matrix U, assuming U is Hermitian.

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According to the spectral theorem for self-adjoint operators you can find a matrix P such that P[tex]^{-1}[/tex]AP is diagonal, i.e. P[tex]^{T}[/tex]AP (P can be shown to be orthogonal). I'm not sure what the result is if the same can be done for the following square (size n X n) and symmetric matrix of the form:
A=
[ U 0 U ]
[ 0 0 0 ]
[ U 0 U ]

where U is square matrix and 0 is a matrix of zeros.

If I am not mistaken the solution is that the columns of P are simply the eigenvectors of A? can anyone confirm this?
 
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First if [itex]A[/itex] is Hermitian then [itex]U[/itex] is also Hermitian, then use the transformation,

[tex] \left[ {\begin{array}{*{20}c}<br /> I & 0 & 0 \\<br /> 0 & I & 0 \\<br /> { - I} & 0 & I \\<br /> \end{array}} \right]\left[ {\begin{array}{*{20}c}<br /> U & 0 & U \\<br /> 0 & 0 & 0 \\<br /> U & 0 & U \\<br /> \end{array}} \right]\left[ {\begin{array}{*{20}c}<br /> I & 0 & { - I} \\<br /> 0 & I & 0 \\<br /> 0 & 0 & I \\<br /> \end{array}} \right] = \left[ {\begin{array}{*{20}c}<br /> U & 0 & 0 \\<br /> 0 & 0 & 0 \\<br /> 0 & 0 & 0 \\<br /> \end{array}} \right]<br /> [/tex]

Now, we are back in the business because now it is the case where you start the argument, diagonalization of a self adjoint operator where we diagonalize [itex]U[/itex] now
 

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