Math 502: Abstract Algebra

Homework 13
Lawrence Tyler Rush
<me@tylerlogic.com>
January 5, 2014
http://coursework.tylerlogic.com/courses/upenn/math502/homework13

1


We first lay out a helpful lemma. 1

Lemma 1.1. Let V be a vector space over F where F is or . If S and T are hermitian and ST = TS, then there is an orthogonal basis for S and T.

Proof. Let λ be an eigenvalue of T and set W to be the eigenspace with respect to lambda. Then the commutativity of ST and TS gives us that

T Sw = ST w = S (λw) = λ(Sw )

for w W. In other words Sw W, implying that W is S-invariant. Now since T is hermitian, then W is 1-dimensional, implying that lambda is an eigenvalue for S and furthermore the eigenspace for S corresponding to λ is W. Since λ is arbitrary and both S and T are diagonalizable, then we know that there exists an orthogonal basis v1,⋅⋅⋅,vn. __

Now for the main event. Let V be a vector space over F where F is or . Also let (⋅|⋅)1 and (⋅|⋅)2 be two distinct inner products on V . Due to Gram-schmitt, we can assume that (⋅|⋅)1 is simply the standard inner product on V . So Then there exists hermitian, positive definite operators T EndF(V ) such that (x|y)2 = (Tx|y)1, and in the case of (⋅|⋅)1, the hermitian operator corresponding to it is Id. Certainly T Id and IdT are commutative and T and Id are both hermitian. Hence Lemma 1.1 implies that we can find an orthogonal basis for the standard inner product, i.e. (⋅|⋅)1, but because (x|y)2 = (Tx|y)1, then this will be othogonal with respect to both inner products.

2


(a)


(b)


Let w Ker(S - λIdW) then we have that (S - λIdW)w = 0, and so Sw = Tw = λw, which implies that w W(λ).

Now assume that w W(λ), then Sw = Tw = λw, which implies that w Ker(S - λIdW).

Hence Ker(S - λIdW) = W(λ).

(c)


We first factor S2 - (λ -λ)S + λλIdW.
  2      --     --         2       --    --
S  - (λ- λ)S +λ λIdW  =   S - λS - λS +-λλIdW
                      =   S(S - λ IdW)- λ (S - λIdW )
                      =   (S - λ-IdW )(S - λ IdW )
First assume that w W(λ) + W(λ), then w = u + v where u W(λ) and v W(λ). But then u and v is killed by (S -λIdW) and (S - λIdW)w, respectively. Hence u + v = w is killed by (S -λIdW)(S - λIdW)w.

Now assume that w Ker(S2 - (λ -λ)S + λλIdW) = Ker((S -λIdW)(S - λIdW)).

(d)


3


Define Q(v) as a quadratic form on n by
Q(x ,...,x ) =  ∑   a  xx
   1     n   1≤i,j≤n ij i j

for some symmetric A = (aij) Mn(). Let λ1 λ2 ⋅⋅⋅λn be the eigenvalues of A with possible multiplicity.

(a) Show that λ1 = max{Q(v) | v n,(v|v) = 1}


Because A is symmetric, we can obtain an orthonormal basis β = {v1,,vn} with respect to the dot product corresponding to the eigenvalues λ1,n. Then for any v n we have v = b1v1 + ⋅⋅⋅ + bnvn which implies
Q (v)  =  (Av|v)
      =  (b1λ1v1 + ⋅⋅⋅+ bnλnvn)|v)
      =  (b λ v|v)+ ⋅⋅⋅+ (b λ v |v)
           1 1 1          n n n
      =  (b1λ1v1|b1v1) + ⋅⋅⋅+ (bnλnvn|bnvn)
      =  b21λ1 + ⋅⋅⋅+ b2nλn
with the last two equalities coming to us by way of the orthonormality of β. Now assuming that (v|v) = 1, then
1 = (v|v) = (b1v1 + ⋅⋅⋅+ bnvn|b1v1 + ⋅⋅⋅+ bnvn) = b21 + ⋅⋅⋅+ b2n

again by the orthonormality of β. Hence λ1 b12λ1 + ⋅⋅⋅ + bn2λn, i.e

                   n
λ1 = max {Q(v) | v ∈ ℝ ,(v|v) = 1}

(b) Extra Credit


(c) Extra Credit


4 Extra Credit


5 Extra Credit


References


[HJE03]   Friedberg S. H., Insel A. J., and Spence L. E. Linear Algebra. Prentice Hall, 2003.