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title: 8-6
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5.2

  • Review the box

  • Algebraic multiplicity bounds geometric multiplicity. Take a basis for the eigenspace. Extend.

  • Let TT be a linear operator and λi\lambda_i be distinct eigenvalues. For each λi\lambda_i, let viEλiv_i\in E_{\lambda_i}, then if vi=0\sum v_i=0, each viv_i is zero.

  • Unions of linearly independent subsets from eigenspaces are still linearly independent.

  • Diagonalizable if and only if algebraic multiplicity equals geometric multiplicity.

    • Proof: Let mim_i be algebraic multiplicity, did_i be geometric multiplicity, and n=dimVn=\dim V.

      Suppose diagonalizable. Then let B be a basis consisting of eigenvectors. Intersect this basis with each eigenspace. Call it BiB_i. Let ni=Bin_i=B_i. Then nnidiminn\leq \sum n_i \leq \sum d_i \leq \sum m_i \leq n.

      So (midi)=0\sum (m_i-d_i)=0. But each term must be nonnegative.

      Conversely, suppose the multiplicties are equal. Then take union of eigenbasis. They form a basis for full space.

  • Testing diagonalizability. Check splitting, check multiplicities. This also computes the diagonalization along the way.

  • What are eigenvalues of derivative?

  • Finite dimensional matrices always have eigenvalues if you extend the field.

  • Give example of infinite dimension transform with no eigenvalues.

  • Work through example 6 in book.

Direct sums

  • Define direct sum

  • Give example

  • Show Jasper's example to motivate

  • Diagonalizable if and only if direct sum of eigenspaces

  • The following are equivalent:

    • direct sum

    • sums and unique way of writing 0

    • unique way of writing any element

    • union of ordered basis for summands is ordered basis

    • exists order basis fof summands so that union is ordered basis.

  • Do more examples