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Mathematics · 术语表

什么是 Diagonalizable, trigonalizable?

又称: diagonalizable · trigonalizable

Definition 3.5 University Mathematics — Year 2 · 第 3 章 — Reduction of Endomorphisms

uu is diagonalizable when EE has a basis of eigenvectors (matrix: similar to a diagonal matrix); trigonalizable when its matrix in some basis is upper triangular.

示例

Example 3.8 (Diagonalization put to work)

A=I+J=(211121112)A = I + J = \left(\begin{smallmatrix}2 & 1 & 1\\ 1 & 2 & 1\\ 1 & 1 & 2\end{smallmatrix}\right), with JJ the all-ones matrix: from Sp⁡(J)={3,0}\operatorname{Sp}(J) = \{3, 0\} (Example 2.19), Sp⁡(A)={4,1}\operatorname{Sp}(A) = \{4, 1\}, with eigenspaces R(1,1,1)\R(1,1,1) and the plane {x+y+z=0}\{x + y + z = 0\}: dimensions 1+2=31 + 2 = 3, diagonalizable (Theorem 3.6 (2)). Powers without any change-of-basis matrix: with Π=J/3\Pi = J/3 the projector onto R(1,1,1)\R(1,1,1),

A=4 Π+1⋅(I−Π)⟹Ak=4k Π+(I−Π)=4k−13 J+I.A = 4\,\Pi + 1\cdot(I - \Pi) \quad\Longrightarrow\quad A^k = 4^k\,\Pi + (I - \Pi) = \frac{4^k - 1}{3}\,J + I .

(Check k=1k = 1: 4−13J+I=A\frac{4-1}3 J + I = A.) The closing insight: when the eigenspaces are visible, spectral projectors compute powers faster than PDP−1PDP^{-1} ever will — and the formula displays the dynamics: AkA^k grows like 4k4^k along (1,1,1)(1,1,1) and stays put on the orthogonal plane.

Example 3.10 (Trigonalizing by hand)

B=(3−111)B = \begin{pmatrix}3 & -1\\ 1 & 1\end{pmatrix}: χB=X2−4X+4=(X−2)2\chi_B = X^2 - 4X + 4 = (X - 2)^2, and ker⁡(B−2I)=ker⁡(1−11−1)\ker(B - 2I) = \ker\left(\begin{smallmatrix}1 & -1\\ 1 & -1\end{smallmatrix}\right) is the line spanned by e1′=(1,1)e_1' = (1, 1): one eigenvalue, a one-dimensional eigenspace — not diagonalizable, but trigonalizable (Theorem 3.9). Complete the basis with e2′=(1,0)e_2' = (1, 0) and compute:

u(e1′)=(2,2)=2e1′,u(e2′)=(3,1)=1⋅e1′+2 e2′,u(e_1') = (2, 2) = 2e_1', \qquad u(e_2') = (3, 1) = 1\cdot e_1' + 2\, e_2' ,

so in the basis (e1′,e2′)(e_1', e_2') the matrix is T=(2102)T = \left(\begin{smallmatrix}2 & 1\\ 0 & 2\end{smallmatrix}\right). The closing insight: the diagonal of TT was forced (both entries must be the double eigenvalue 22); only the corner entry depended on the choice of e2′e_2', and rescaling e2′e_2' can make it any nonzero value — the resistant “11” is the shadow of the nilpotent part that Dunford will isolate.

Example 3.4 (Same χ\chi, different geometry)

The matrices

(2002)and(2102)\begin{pmatrix}2 & 0\\ 0 & 2\end{pmatrix} \qquad\text{and}\qquad \begin{pmatrix}2 & 1\\ 0 & 2\end{pmatrix}

share the characteristic polynomial (X−2)2(X - 2)^2, the trace, the determinant, the spectrum — yet are not similar: the first has E2E_2 of dimension 22 (geometric multiplicity 22), the second of dimension 11. The characteristic polynomial sees only algebraic multiplicities; the eigenspace dimensions are the finer invariant, and the minimal polynomial arbitrates (X−2X - 2 versus (X−2)2(X - 2)^2). Moral for all diagonalizability discussions: χ\chi shortlists the candidates, but kernels cast the votes.

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