Let TEL(V) be self-adjoint. Let A₁, A2,..., Am be the distinct eigen- values of T. For i = 1, 2, ..., m, let E; := E(\¿,T) be the corresponding eigenspace, and let PrĒ; € L(V) denote the orthogonal projection onto E¿. a.) Prove that for any 1 ≤i, j≤m, b.) Prove that Pre; Pre; = dij PrEi · T = A₁ PrE₁ +₂ PrE₂ + + Am PrEm. Equation (1) is called the spectral decomposition of T. (1)
Let TEL(V) be self-adjoint. Let A₁, A2,..., Am be the distinct eigen- values of T. For i = 1, 2, ..., m, let E; := E(\¿,T) be the corresponding eigenspace, and let PrĒ; € L(V) denote the orthogonal projection onto E¿. a.) Prove that for any 1 ≤i, j≤m, b.) Prove that Pre; Pre; = dij PrEi · T = A₁ PrE₁ +₂ PrE₂ + + Am PrEm. Equation (1) is called the spectral decomposition of T. (1)
Let TEL(V) be self-adjoint. Let A₁, A2,..., Am be the distinct eigen- values of T. For i = 1, 2, ..., m, let E; := E(\¿,T) be the corresponding eigenspace, and let PrĒ; € L(V) denote the orthogonal projection onto E¿. a.) Prove that for any 1 ≤i, j≤m, b.) Prove that Pre; Pre; = dij PrEi · T = A₁ PrE₁ +₂ PrE₂ + + Am PrEm. Equation (1) is called the spectral decomposition of T. (1)
Branch of mathematics concerned with mathematical structures that are closed under operations like addition and scalar multiplication. It is the study of linear combinations, vector spaces, lines and planes, and some mappings that are used to perform linear transformations. Linear algebra also includes vectors, matrices, and linear functions. It has many applications from mathematical physics to modern algebra and coding theory.
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