Verify Cayley-Hamilton theorem of A= ( 1 2 2 3 1 0 1 1 1 )
"P_A(\\lambda)=\\det(A-\\lambda I)=\\begin{vmatrix}\n 1-\\lambda & 2 & 2 \\\\\n 3 & 1-\\lambda & 0 \\\\\n 1 & 1 & 1-\\lambda \\\\\n\\end{vmatrix}"
"=(1-\\lambda)\\begin{vmatrix}\n 1-\\lambda & 0 \\\\\n 1 & \\lambda-1\n\\end{vmatrix}-2\\begin{vmatrix}\n 3 & 0 \\\\\n 1 & 1-\\lambda\n\\end{vmatrix}"
"+2\\begin{vmatrix}\n 3 & 1-\\lambda \\\\\n 1 & 1\n\\end{vmatrix}=(1-\\lambda)^3-6(1-\\lambda)+6-2(1-\\lambda)"
"=1-3\\lambda+3\\lambda^2-\\lambda^3-8+8\\lambda+6"
"=-\\lambda^3+3\\lambda^2+5\\lambda-1"
"A^2=\\begin{pmatrix}\n 1 & 2 & 2 \\\\\n 3 & 1 & 0 \\\\\n 1 & 1 & 1 \\\\\n\\end{pmatrix}\\begin{pmatrix}\n 1 & 2 & 2 \\\\\n 3 & 1 & 0 \\\\\n 1 & 1 & 1 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n 1+6+2 & 2+2+2 & 2+0+2 \\\\\n 3+3+0 & 6+1+0 & 6+0+0 \\\\\n 1+3+1 & 2+1+1 & 2+0+1 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n 9 & 6 & 4 \\\\\n 6 & 7 & 6 \\\\\n 5 & 4 & 3 \\\\\n\\end{pmatrix}"
"A^3=\\begin{pmatrix}\n 9 & 6 & 4 \\\\\n 6 & 7 & 6 \\\\\n 5 & 4 & 3 \\\\\n\\end{pmatrix}\\begin{pmatrix}\n 1 & 2 & 2 \\\\\n 3 & 1 & 0 \\\\\n 1 & 1 & 1 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n 9+18+4 & 18+6+4 & 18+0+4 \\\\\n 6+21+6 & 12+7+6 & 12+0+6 \\\\\n 5+12+3 & 10+4+3 & 10+0+3 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n 31 & 28 & 22 \\\\\n 33 & 25 & 18 \\\\\n 20 & 17 & 13 \\\\\n\\end{pmatrix}"
"-A^3+3A^2+5A-I=-\\begin{pmatrix}\n 31 & 28 & 22 \\\\\n 33 & 25 & 18 \\\\\n 20 & 17 & 13 \\\\\n\\end{pmatrix}"
"+3\\begin{pmatrix}\n 9 & 6 & 4 \\\\\n 6 & 7 & 6 \\\\\n 5 & 4 & 3 \\\\\n\\end{pmatrix}+5\\begin{pmatrix}\n 1 & 2 & 2 \\\\\n 3 & 1 & 0 \\\\\n 1 & 1 & 1 \\\\\n\\end{pmatrix}-\\begin{pmatrix}\n 1 & 0 & 0 \\\\\n 0 & 1 & 0 \\\\\n 0 & 0 & 1 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n -31+27+5-1 & -28+18+10-0 & -22+12+10-0 \\\\\n -33+18+15-0 & -25+21+5-1 & -18+18+0-0 \\\\\n -20+15+5-0 & -17+12+5-0 & -13+9+5-1 \\\\\n\\end{pmatrix}"
"=\\begin{pmatrix}\n 0 & 0 & 0 \\\\\n 0 & 0 & 0 \\\\\n 0 & 0 & 0 \\\\\n\\end{pmatrix}"
The matrix "A" satisfies its own characteristic equation.
Therefore we verify Cayley-Hamilton theorem of "A=\\begin{pmatrix}\n 1 & 2 & 2 \\\\\n 3 & 1 & 0 \\\\\n 1 & 1 & 1 \\\\\n\\end{pmatrix}."
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