A matrix is diagonalizable when algebraic and geometric multiplicities are equal

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SUMMARY

A matrix is diagonalizable if and only if its algebraic and geometric multiplicities are equal. This means there exists a complete set of eigenvectors for the matrix, allowing for a basis of the vector space U to consist entirely of these eigenvectors. The algebraic multiplicity refers to the size of the matrix, while the geometric multiplicity indicates the number of independent eigenvectors. To construct the matrix representing a linear transformation, apply the transformation to each basis vector and express the result as a linear combination of basis vectors.

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A matrix is diagonalizable when algebraic and geometric multiplicities are equal.
I know this is true, and my professor proved it, but I did not understand him fully. Can someone please explain?
 
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This area is for "Learning Materials", not questions. I am moving this thread to "Linear and Abstract Algebra".
 
A matrix is diagonalizable if and only if there exist a "complete set" of eigenvectors. (Your "algebraic and geometric multiplicities are equal". The algebraic multiplicity is the size of the matrix, the geometric multiplicity is the number of independent eigenvectors.) Specifically, if the matrix represents a linear transformation on vector space U, then, in order to be "diagonalizable", there must exist a basis for U consisting of eigenvectors of the linear transformation. You construct the matrix representing a linear transformation, in a given basis, by applying the transformation to each basis vector in turn, writing the result as a linear combination of basis vectors. The coefficients give each column of the matrix.

If all the basis vectors \{v_1, v_2, \cdot\cdot\cdot\, v_n\} are eigenvectors, that is, if Lv_1= \lambda_1v_1, Lv_2= \lamba_2v_2, \cdot\cdot\cdot, Lv_n= \lambda_nv_n, then each column consists of the eigenvalue, in the appropriate position, and "0"s:
\begin{bmatrix}\lambda_1 & 0 & \cdot & \cdot & \cdot & 0 \\ 0 & \lambda_2 & \cdot & \cdot\ & \cdot & 0 \\ \cdot & \cdot\ & \cdot\ & \cdot & \cdot & \cdot \\ 0 & 0 & \cdot & \cdot & \cdot & \lambda_n\end{bmatrix}
 

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