6. a) Given any real symmetric square matrix A of order n, show that the function RnxRn "\\to" defined by I(x, y) =xTAy is a symmetric bilinear function
Give examples of matrices A for which the corresponding I is not an inner product
State the extra properties on A which would make the corresponding I an inner product
b) Show that R[x] deg ≤ 2 x R[x] deg ≤ 2 defined by I (p(x), q(x)) =p(0)q(0)+p(1/2)q(1/2)+p(1)q(1) is an inner product on R[x] deg ≤ 2
Use Gram-Schmidt procedure to obtain a orthogonal basis of R[x] deg ≤ 2(with respect to the inner product defined above) which contains the polynomial x
The function defined by "\\Iota(x,y) = x^TAy" is a symmetric bilinear function
1) it satisfies the axiom <u,v> = <v,u> in such:
⟨x,y⟩=x"^T" Ay=x⋅(Ay)
Since A is symmetric
⟨x,y⟩=x⋅(Ay)=(Ay)⋅x
=(Ay)"^T"x=y"^T" A"^T" x=y"^T" Ax=⟨y,x⟩.
(ii) For any vector x,y,z and any real number r, we have:
"\\langle rx,y\\rangle=(rx)^TAy=rx^TAy=r\\langle x,y\\rangle"
and
"\\langle\\>x+y,z\\rangle=(x+y)^TAz=(x^T+y^T)Az"
"=x^TAz+y^TAz=\\langle\\>x,y\\rangle=\\langle\\>y,z\\rangle"
Therefore the linearity in the first argument is satisfied
It satisfies the rule of positive- Definiteness in such
If "x\\ne0" then we have
"\\langle\\>x,x\\rangle=x^TAx>0"
Examples of matrices A for which the corresponding "\\Iota" is not an inner product
"\\to \\>" A matrix of order m"\u00d7"n
"\\to" A matrix A "\\ne\\>A^T"
"\\to" A matrix A whose eigenvalues "\\lambda\\> \\leq0"
"\\to" A matrix A whose determinant det "A=0"
Properties of A which would make the corresponding "\\Iota" on inner product
Matrix A should be a real symmetric "n\u00d7n" matrix
Matrix A must be positive definite in that
"x^TAx>0"
Matrix A has real eigenvalues
The eigenvectors of matrix A corresponding to the eigenvalues are orthogonal
Matrix A is diagonalizable
Part 6(B) sections
"\\Iota" is inner product if it satisfies conjugate symmetry, linearity and positive Definiteness axioms
(I) "<q(x),p(x)>=q(0)p(0)+q(\\frac{1}{2})q(\\frac{1}{2})+q(1)p(1)"
"=p(0)q(0)+p(\\frac{1}{2})q(\\frac{1}{2})+p(1)q(1)"
"\\therefore<q(x),p(x)>=<p(x),q(x)>"
"\\Iota" is symmetric
(ii) "c<p,q>=c\\>[{p(0)q(0)+p(\\frac{1}{2}q(\\frac{1}{2}+p(1)q(1)}]"
"=cp(0)q(0)+cp(\\frac{1}{2})q(\\frac{1}{2})+cp(1)q(1)"
"=<cpf,q>"
"\\Iota" satisfies linearity
(iii) "<p,p>=p(0)p(0)+p(\\frac{1}{2})p(\\frac{1}{2})+p(1)p(1)>0"
If "p(x)" is not zero
Part 6(B) section 2
The standard polynomial basis for "R[x]deg\\>\\le2" is defined "[1,x,x^2]"
Let orthogonal basis of "\\Iota" be "(b_1,b_2,b_3)"
"b_1=1"
"b_2=x-proj_1x"
"\\therefore b_2=x-\\frac{<1,x>}{<1,1>}1"
"<1,x>=(1)(0)+(1)(\\frac{1}{2})+(1)(1)=\\frac{3}{2}"
"<1,1>=(1)(1)+(1)(1)+(1)(1)=3"
"b_2=x-\\frac{1}{2}"
"b_3=x^2-\\frac{<x^2,1>}{<1,1>}1-" "\\frac{<x^2,x-\\frac{1}{2}>}{<x-\\frac{1}{2},x-\\frac{1}{2}>}(x-\\frac{1}{2})"
"<x^2,1>=(1)(0)+(1)(\\frac{1}{2})^2+(1)(1)^2=\\frac{5}{4}"
"<x-\\frac{1}{2},x-\\frac{1}{2}>=(\\frac{-1}{2})(\\frac{-1}{2})+(0)(0)+(\\frac{1}{2})(\\frac{1}{2})=\\frac{1}{2}"
"<x^2,x-\\frac{1}{2}>=(0)(\\frac{-1}{2})+(^\\frac{1}{2})^2(0)+(1)^2(\\frac{1}{2})"
"=\\frac{1}{2}"
"b_3=x^2-\\frac{5}{12}-1(x-\\frac{1}{2})"
"=x^2-x+\\frac{1}{12}"
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