第17章 17.23

(1)

a≠0a \neq 0 のとき

∣A−λI∣=∣1−λaaa1−λaaa1−λ∣=(1−λ)3+2a3−3a2(1−λ)=−λ3+3λ2+3(a2−1)λ+2a3−3a2+1|A - \lambda I| = \begin{vmatrix} 1-\lambda & a & a \\ a & 1-\lambda & a \\ a & a & 1-\lambda \end{vmatrix} = (1-\lambda)^3 + 2a^3 - 3a^2(1-\lambda) = -\lambda^3 + 3\lambda^2 + 3(a^2-1)\lambda + 2a^3 - 3a^2 + 1

=−λ3+3λ2+3(a2−1)λ−(1−a)2(1+2a)=−{λ−(1−a)}2{λ−(1+2a)}=0= -\lambda^3 + 3\lambda^2 + 3(a^2-1)\lambda - (1-a)^2(1+2a) = -\{\lambda - (1-a)\}^2\{\lambda - (1+2a)\} = 0

∴λ=1+2a,1−a(重解)\therefore \lambda = 1 + 2a, 1 - a \text{(\text{重解})}

λ=1+2a\lambda = 1 + 2a のとき

(−2aaaa−2aaaa−2a)⇒(−2aaa2a−4a2a2a2a−4a)⇒(−2aaa0−3a3a03a−3a)⇒(−2aaa01−1000)\begin{pmatrix} -2a & a & a \\ a & -2a & a \\ a & a & -2a \end{pmatrix} \Rightarrow \begin{pmatrix} -2a & a & a \\ 2a & -4a & 2a \\ 2a & 2a & -4a \end{pmatrix} \Rightarrow \begin{pmatrix} -2a & a & a \\ 0 & -3a & 3a \\ 0 & 3a & -3a \end{pmatrix} \Rightarrow \begin{pmatrix} -2a & a & a \\ 0 & 1 & -1 \\ 0 & 0 & 0 \end{pmatrix}

⇒(−2a02a01−1000)⇒(10−101−1000)\Rightarrow \begin{pmatrix} -2a & 0 & 2a \\ 0 & 1 & -1 \\ 0 & 0 & 0 \end{pmatrix} \Rightarrow \begin{pmatrix} 1 & 0 & -1 \\ 0 & 1 & -1 \\ 0 & 0 & 0 \end{pmatrix}

∴P1=(111)\therefore P_1 = \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}

単位ベクトルにすると P1′=13(111)P_1' = \frac{1}{\sqrt{3}} \begin{pmatrix} 1 \\ 1 \\ 1 \end{pmatrix}

λ=1−a\lambda = 1 - a のとき

(aaaaaaaaa)⇒(111000000)\begin{pmatrix} a & a & a \\ a & a & a \\ a & a & a \end{pmatrix} \Rightarrow \begin{pmatrix} 1 & 1 & 1 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix}

∴P2=(−110),P3=(−101)\therefore P_2 = \begin{pmatrix} -1 \\ 1 \\ 0 \end{pmatrix}, P_3 = \begin{pmatrix} -1 \\ 0 \\ 1 \end{pmatrix}

単位ベクトルにすると P2′=12(−110),P3′=12(−101)P_2' = \frac{1}{\sqrt{2}} \begin{pmatrix} -1 \\ 1 \\ 0 \end{pmatrix}, P_3' = \frac{1}{\sqrt{2}} \begin{pmatrix} -1 \\ 0 \\ 1 \end{pmatrix}

これからP=(13−12−121312013012)\text{これから} \quad P = \begin{pmatrix} \frac{1}{\sqrt{3}} & -\frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \\ \frac{1}{\sqrt{3}} & \frac{1}{\sqrt{2}} & 0 \\ \frac{1}{\sqrt{3}} & 0 & \frac{1}{\sqrt{2}} \end{pmatrix}

(P−1AP=(1+2a0001−a0001−a))\left(P^{-1}AP = \begin{pmatrix} 1+2a & 0 & 0 \\ 0 & 1-a & 0 \\ 0 & 0 & 1-a \end{pmatrix}\right)

a=0a = 0 のとき

∣A−λE∣=∣1−λ0001−λ0001−λ∣=(1−λ)3=0|A - \lambda E| = \begin{vmatrix} 1-\lambda & 0 & 0 \\ 0 & 1-\lambda & 0 \\ 0 & 0 & 1-\lambda \end{vmatrix} = (1-\lambda)^3 = 0

∴λ=1(三重解)\therefore \lambda = 1 \text{(\text{三重解})}

λ=1\lambda = 1 のとき

(000000000)\begin{pmatrix} 0 & 0 & 0 \\ 0 & 0 & 0 \\ 0 & 0 & 0 \end{pmatrix}

よって任意の直交行列でよい

(2)

txAx=(xyz)(1aaa1aaa1)(xyz)=(x+ay+azax+y+azax+ay+z)(xyz){}^t xAx = (x \quad y \quad z) \begin{pmatrix} 1 & a & a \\ a & 1 & a \\ a & a & 1 \end{pmatrix} \begin{pmatrix} x \\ y \\ z \end{pmatrix} = (x + ay + az \quad ax + y + az \quad ax + ay + z) \begin{pmatrix} x \\ y \\ z \end{pmatrix}

=(x+ay+az)(x+y+z)+(ax+y+az)(x+y+z)+(ax+ay+z)(x+y+z)= (x + ay + az)(x + y + z) + (ax + y + az)(x + y + z) + (ax + ay + z)(x + y + z)

=(x+y+z){(1+2a)x+(1+2a)y+(1+2a)z}=(1+2a)(x+y+z)2>0= (x + y + z)\{(1 + 2a)x + (1 + 2a)y + (1 + 2a)z\} = (1 + 2a)(x + y + z)^2 > 0

(x+y+z)2>0(x + y + z)^2 > 0 から 1+2a>01 + 2a > 0 であればよいので −12<a-\dfrac{1}{2} < a

解説: r31bn1z