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東京大学 新領域創成科学研究科 メディカル情報生命専攻 2022年8月実施 問題8

Author

zephyr

Description

(1) Describe the eigenvalues and eigenvectors of the following matrix. (λ\lambda is a real value.)

Aλ=(λ111λ111λ)\mathbf{A}_\lambda = \begin{pmatrix} \lambda & 1 & 1 \\ 1 & \lambda & 1 \\ 1 & 1 & \lambda \end{pmatrix}

(2) What is the range of λ\lambda such that Aλ\mathbf{A}_\lambda is positive semidefinite.

(3) Consider an n×nn \times n symmetric matrix where all diagonal elements are bb and all non-diagonal elements are aa. Show that this matrix is non-singular when b>(n1)a|b| > |(n - 1)a|.

题目描述

  1. 对实参数 λ\lambda,求矩阵
    Aλ=(λ111λ111λ)\mathbf A_\lambda= \begin{pmatrix} \lambda&1&1\\ 1&\lambda&1\\ 1&1&\lambda \end{pmatrix}
    的全部特征值及相应特征向量。
  2. 求使 Aλ\mathbf A_\lambda 为半正定矩阵的 λ\lambda 取值范围。
  3. 设一个 n×nn\times n 对称矩阵的全部对角元均为 bb,全部非对角元均为 aa。证明当
    b>(n1)a|b|>|(n-1)a|
    时该矩阵非奇异。

考点

  • 高对称矩阵的特征分解:把全一方向与其正交补分开,求常对角、常非对角矩阵的两个特征值及特征空间。
  • 半正定判定:利用实对称矩阵全部特征值非负的充要条件,确定参数 λ\lambda 的范围。
  • 严格对角占优:由 b>(n1)a|b|>(n-1)|a| 或等价谱表达证明零不可能成为特征值,从而得到非奇异性。

Kai

(1) Eigenvalues and Eigenvectors

To find the eigenvalues μi\mu_i of the matrix Aλ\mathbf{A}_\lambda, we need to solve the characteristic equation det(AλμI)=0\det(\mathbf{A}_\lambda - \mu \mathbf{I}) = 0.

AλμI=(λμ111λμ111λμ)\mathbf{A}_\lambda - \mu \mathbf{I} = \begin{pmatrix} \lambda - \mu & 1 & 1 \\ 1 & \lambda - \mu & 1 \\ 1 & 1 & \lambda - \mu \end{pmatrix}

Using the row addition method for simplification, we can add all rows to the first row:

λμ111λμ111λμ=λμ+1+11+(λμ)+11+1+(λμ)1λμ111λμ=λμ+2λμ+2λμ+21λμ111λμ\begin{vmatrix} \lambda - \mu & 1 & 1 \\ 1 & \lambda - \mu & 1 \\ 1 & 1 & \lambda - \mu \end{vmatrix} = \begin{vmatrix} \lambda - \mu + 1 + 1 & 1 + (\lambda - \mu) + 1 & 1 + 1 + (\lambda - \mu) \\ 1 & \lambda - \mu & 1 \\ 1 & 1 & \lambda - \mu \end{vmatrix} = \begin{vmatrix} \lambda - \mu + 2 & \lambda - \mu + 2 & \lambda - \mu + 2 \\ 1 & \lambda - \mu & 1 \\ 1 & 1 & \lambda - \mu \end{vmatrix}

Now, we can absorb the common factor (λμ+2)(\lambda - \mu + 2) from the first row:

=(λμ+2)1111λμ111λμ=(λμ+2)1110λμ1000λμ1=(λμ+2)(λμ1)2= (\lambda - \mu + 2) \begin{vmatrix} 1 & 1 & 1 \\ 1 & \lambda - \mu & 1 \\ 1 & 1 & \lambda - \mu \end{vmatrix} = (\lambda - \mu + 2) \begin{vmatrix} 1 & 1 & 1 \\ 0 & \lambda - \mu - 1 & 0 \\ 0 & 0 & \lambda - \mu - 1 \end{vmatrix} = (\lambda - \mu + 2)(\lambda - \mu - 1)^2

Setting the determinant to zero:

So, the eigenvalues are:

μ1=λ+2,μ2=λ1(with multiplicity 2)\mu_1 = \lambda + 2, \quad \mu_2 = \lambda - 1 \quad \text{(with multiplicity 2)}

Eigenvectors

For μ1=λ+2\mu_1 = \lambda + 2:

Aλ(λ+2)I=(211121112)\mathbf{A}_\lambda - (\lambda + 2) \mathbf{I} = \begin{pmatrix} -2 & 1 & 1 \\ 1 & -2 & 1 \\ 1 & 1 & -2 \end{pmatrix}

Solving

(211121112)v=0\begin{pmatrix} -2 & 1 & 1 \\ 1 & -2 & 1 \\ 1 & 1 & -2 \end{pmatrix} \mathbf{v} = \mathbf{0}

, we find:

v1=(111)\mathbf{v}_1 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}

For μ2=λ1\mu_2 = \lambda - 1:

Aλ(λ1)I=(111111111)\mathbf{A}_\lambda - (\lambda - 1) \mathbf{I} = \begin{pmatrix} 1 & 1 & 1 \\ 1 & 1 & 1 \\ 1 & 1 & 1 \end{pmatrix}

We need to solve Aλv=(λ1)v\mathbf{A}_\lambda \mathbf{v} = (\lambda - 1)\mathbf{v}, which gives the eigenvectors corresponding to μ2\mu_2. This generally results in two linearly independent eigenvectors orthogonal to v1\mathbf{v}_1:

v2=(101),v3=(011)\mathbf{v}_2 = \begin{pmatrix} 1 \\ 0 \\ -1 \end{pmatrix}, \quad \mathbf{v}_3 = \begin{pmatrix} 0 \\ 1 \\ -1 \end{pmatrix}

(2) Positive Semi-definiteness

A matrix is positive semidefinite if all its eigenvalues are non-negative. For Aλ\mathbf{A}_\lambda to be positive semidefinite:

μ1=λ+20\mu_1 = \lambda + 2 \geq 0
μ2=λ10\mu_2 = \lambda - 1 \geq 0

Solving these inequalities:

λ+20    λ2\lambda + 2 \geq 0 \implies \lambda \geq -2
λ10    λ1\lambda - 1 \geq 0 \implies \lambda \geq 1

The most restrictive condition is λ1\lambda \geq 1.

Thus, the range of λ\lambda such that Aλ\mathbf{A}_\lambda is positive semidefinite is:

λ1\lambda \geq 1

(3) Non-Singularity of Symmetric Matrix

Consider an n×nn \times n symmetric matrix B\mathbf{B} where all diagonal elements are bb and all non-diagonal elements are aa.

B=(baaaabaaaabaaaab)\mathbf{B} = \begin{pmatrix} b & a & a & \cdots & a \\ a & b & a & \cdots & a \\ a & a & b & \cdots & a \\ \vdots & \vdots & \vdots & \ddots & \vdots \\ a & a & a & \cdots & b \end{pmatrix}

The matrix B\mathbf{B} can be written as:

B=bI+aJ\mathbf{B} = b\mathbf{I} + a\mathbf{J}

where J\mathbf{J} is the n×nn \times n matrix with all elements equal to 1.

The eigenvalues of J\mathbf{J} are nn (with multiplicity 1) and 00 (with multiplicity n1n-1). Thus, the eigenvalues of B\mathbf{B} are:

λ1=b+(n1)aandλ2=ba(with multiplicity n1)\lambda_1 = b + (n-1)a \quad \text{and} \quad \lambda_2 = b - a \quad (\text{with multiplicity } n-1)

The matrix B\mathbf{B} is non-singular if all its eigenvalues are non-zero:

b+(n1)a0b + (n-1)a \neq 0
ba0b - a \neq 0

This holds if:

b>(n1)a|b| > |(n-1)a|

since b>(n1)a|b| > (n-1)|a| implies b>a|b| > |a| when n2n \geq 2.

Thus, the matrix B\mathbf{B} is non-singular when b>(n1)a|b| > |(n-1)a|.

Knowledge

特征值和特征向量 正定矩阵

难点解题思路

  1. 通过求解特征方程来找到特征值。
  2. 根据特征值的符号判断矩阵的半正定性。
  3. 使用矩阵特征值的性质判断矩阵的非奇异性。

解题技巧和信息

  1. 计算特征方程时,使用行列式和代数余子式。
  2. 确定半正定矩阵时,所有特征值必须为非负数。
  3. 判断矩阵是否非奇异,可以通过特征值是否全非零来实现。

重点词汇

eigenvalue 特征值

eigenvector 特征向量

positive semidefinite 正半定

non-singular 非奇异

参考资料

  1. Linear Algebra and Its Applications by Gilbert Strang, Chap. 6
  2. Introduction to Linear Algebra by Gilbert Strang, Chap. 7