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Diagonalizability of Linear Transformations, Multiplicity of Eigenvalues, and the Relationship with Eigenspaces 📂Linear Algebra

Diagonalizability of Linear Transformations, Multiplicity of Eigenvalues, and the Relationship with Eigenspaces

Theorem1

Let T:VVT : V \to V be a linear transformation on a finite-dimensional vector space VV. Suppose the characteristic polynomial of TT splits and λ1,λ2,,λk\lambda_{1}, \lambda_{2}, \dots, \lambda_{k} are distinct eigenvalues of TT. Then,

  1. TT is diagonalizable if and only if, for all ii, the multiplicity of λi\lambda_{i} and the dimension dim(Eλi)\dim(E_{\lambda_{i}}) of the eigenspace are the same.
    T is diagobalizable.     multiplicity of λi=dim(Eλi),i T \text{ is diagobalizable. } \iff \text{multiplicity of } \lambda_{i} = \dim(E_{\lambda_{i}}),\quad \forall i

  2. If TT is diagonalizable, and if βi\beta_{i} is an ordered basis of EλiE_{\lambda_{i}}, then β=β1βk\beta = \beta_{1} \cup \cdots \cup \beta_{k} is an ordered basis of VV containing the eigenvectors of TT.

  3. TT is diagonalizable if and only if VV is the direct sum of the eigenspaces of TT. T is diagobalizable.     V=Eλ1Eλk T \text{ is diagobalizable. } \iff V = E_{\lambda_{1}} \oplus \cdots \oplus E_{\lambda_{k}}

Proof

1.

Let mim_{i} be the multiplicity of λi\lambda_{i}. Suppose di=dim(Eλi)d_{i} = \dim(E_{\lambda_{i}}), n=dim(V)n = \dim(V).

  • ()(\Longrightarrow)

    Assume TT is diagonalizable. This is equivalent to saying that there exists a basis of VV consisting of the eigenvectors of TT. Let β\beta be such a basis of VV, consisting of the eigenvectors of TT. For each ii, let βi=βEλi\beta_{i} = \beta \cap E_{\lambda_{i}}. In other words, βi\beta_{i} is a set of eigenvectors corresponding to the eigenvalue λi\lambda_{i} that belong to β\beta. Also, suppose ni=βin_{i} = \left| \beta_{i} \right|. Then, since βi\beta_{i} is a linearly independent subset of EλiE_{\lambda_{i}}, nidin_{i} \le d_{i} holds. Moreover, since the algebraic multiplicity of an eigenvalue is greater or equal to its geometric multiplicity, dimid_{i} \le m_{i} holds. Therefore, n=βn = \left| \beta \right| implies, by adding nin_{i} for all ii, we get nn, and by definition of multiplicity, adding mim_{i} for all ii also results in nn. Therefore, n=i=1knii=1kdii=1kmi=n n = \sum\limits_{i=1}^{k}n_{i} \le \sum\limits_{i=1}^{k}d_{i} \le \sum\limits_{i=1}^{k}m_{i} = n     i=1k(midi)=0 \implies \sum\limits_{i=1}^{k}(m_{i} - d_{i}) = 0 But since midi0m_{i} - d_{i} \ge 0, for all ii, mi=dim_{i} = d_{i} holds.

  • ()(\Longleftarrow)

    Suppose that for all ii, mi=dim_{i} = d_{i} holds. Let βi\beta_{i} be an ordered basis of EλiE_{\lambda_{i}}. And let β=β1βk\beta = \beta_{1} \cup \cdots \cup \beta_{k}. Then, because the union of linearly independent sets from different eigenspaces is also linearly independent, β\beta is linearly independent. Also, by assumption, i=1kdi=i=1kmi=n\sum\limits_{i=1}^{k} d_{i} = \sum\limits_{i=1}^{k} m_{i} = n holds, so β\beta contains nn linearly independent eigenvectors. Therefore, β\beta is an ordered basis of VV, and TT is diagonalizable.

2.

The proof of ()(\Longleftarrow) in 1. already covered this.

3.

Let λ1,,λk\lambda_{1}, \dots, \lambda_{k} be distinct eigenvalues of TT.

  • ()(\Longrightarrow)

    Assume TT is diagonalizable. Let γi\gamma_{i} be an ordered basis of the eigenspace EλiE_{\lambda_{i}}. Then, by 2., γ1γk\gamma_{1} \cup \cdots \cup \gamma_{k} is an ordered basis of VV.

    Properties of direct sums

    Let W1,W2,,WkW_{1}, W_{2}, \dots, W_{k} be subspaces of a finite-dimensional vector space VV. The following propositions are equivalent:

    1. V=W1W2WkV = W_{1} \oplus W_{2} \oplus \cdots \oplus W_{k}
    2. If γi\gamma_{i} is an ordered basis of WiW_{i}, then γ1γk\gamma_{1} \cup \cdots \cup \gamma_{k} is an ordered basis of VV.
    3. There exists an ordered basis γi\gamma_{i} of WiW_{i} such that γ1γk\gamma_{1} \cup \cdots \cup \gamma_{k} is an ordered basis of VV. Thus, by the theorem above, V=Eλ1EλkV = E_{\lambda_{1}} \oplus \cdots \oplus E_{\lambda_{k}} holds.
  • ()(\Longleftarrow)

    Assume V=Eλ1EλkV = E_{\lambda_{1}} \oplus \cdots \oplus E_{\lambda_{k}}. Let γi\gamma_{i} be an ordered basis of EλiE_{\lambda_{i}}. Then, by the properties of direct sums, γ1γk\gamma_{1} \cup \cdots \cup \gamma_{k} is an ordered basis of VV. Since this basis consists of eigenvectors, TT is diagonalizable.


  1. Stephen H. Friedberg, Linear Algebra (4th Edition, 2002), p268, ↩︎