Math 2.0

statement theorem

Decomposition into generalised eigenspaces

Statement

Let FF be a field, let VV be a finite-dimensional vector space over FF, and let T ⁣:V→VT \colon V \to V be a linear map. Assume that the characteristic polynomial of TT splits over FF as pT(t)=(t−λ1)m1⋯(t−λk)mkp_T(t) = (t - \lambda_1)^{m_1} \cdots (t - \lambda_k)^{m_k} with pairwise distinct λi\lambda_i. Then V=Vλ1⊕⋯⊕Vλk,V = V_{\lambda_1} \oplus \cdots \oplus V_{\lambda_k}, where VλiV_{\lambda_i} is the generalised eigenspace of λi\lambda_i, and dim⁡Vλi=mi\dim V_{\lambda_i} = m_i.

Remarks

The hypothesis holds for every TT when FF is algebraically closed, for example F=CF = \C. Each VλiV_{\lambda_i} is TT-invariant, and T−λiid⁡T - \lambda_i \id is nilpotent on it. A proof uses the coprime polynomials (t−λi)mi(t - \lambda_i)^{m_i} and the Cayley–Hamilton theorem. This direct sum decomposition is the first step towards the Jordan normal form.

Explanations

L1 human

Over C\C, the space splits into pieces, one for each eigenvalue. On each piece, the map is λ\lambda times the identity plus a nilpotent part. So a hard problem breaks into simpler problems, one for each eigenvalue.

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  1. Vector space definition
  2. Linear map definition
  3. Linear subspace definition
  4. Endomorphism definition
  5. Sum of subspaces definition
  6. Eigenvalue definition
  7. Polynomial of an endomorphism definition
  8. Direct sum of subspaces definition
  9. Eigenvector definition
  10. Generalised eigenvector definition
  11. Generalised eigenspace definition
  12. Decomposition into generalised eigenspaces statement

Sources

  1. Web https://en.wikipedia.org/wiki/Generalized_eigenvector, Jordan normal form