Under an orthogonal change of coordinates represented by , the component matrix changes byThus is similar to , so its characteristic polynomial, eigenvalues, and their algebraic multiplicities are unchanged.
If is symmetric, the spectral theorem for real symmetric matrices makes it diagonalizable, so algebraic and geometric multiplicities agree. Consequently the dimensions of its eigenspaces are also independent of the coordinate frame.
For the stated tensor, choose a unit eigenvector belonging to the simple eigenvalue . Its perpendicular plane is the eigenspace of , soHence
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