Paul K. answered 10/08/20
Math PhD with a passion for sharing knowledge
(a) Recall that for a square matrix M to be symmetric, M = Mτ. We examine G and show that it is equal to its transpose. Gτ = (I - vvτ)τ = Iτ - (vvτ)τ = I - (vτ)τ(v)τ = I - vvτ = G, so G is symmetric.
Now, we expand G2 to show it equals G. Observe that vτv = 〈v,v〉= 1 since v is a unit vector.
G2 = (I - vvτ)(I - vvτ) = I - vvτ - vvτ + vvτvvτ = I - 2vvτ + v(1)vτ = I - 2vvτ + vvτ = I - vvτ = G.
(b) A vector v is an eigenvalue of operator (or square matrix) T if Tv = rv for r a value of the underlying field. We examine Gv. Since v is a unit vector, vτv is equal to 1, so Gv = Iv - vvτv = Iv - v(1) = v - 1v = 0. The eigenvalue is 0.
(c) Suppose that u is a vector such that 〈u,v〉= 0. Since the inner product is symmetric, vτu = 〈v,u〉 = 0, it follows that Gu = Iu - vvτu = u - v(0) = u. Thus u is an eigenvector with eigenvalue 1.
(d) If we can exhibit an basis of Rn consisting of eigenvectors of G, then we can diagonalize G. We already have shown that v is an eigenvector of G and that any vector u orthogonal to v is also an eigenvector. Thus, if we pick v and a basis of the space orthogonal to the subspace spanned by v, we can exhibit such a basis of Rn. Take an orthogonal decomposition of Rn in terms of v ⊕ v⊥ where v⊥ denotes the hyperplane orthogonal to v. Pick a basis u1,...,un-1 of v⊥. By (c), these are all eigenvectors of G with eigenvalue 1. Hence, G written in the basis {v, u1,..., un-1} will be a diagonal matrix with first entry equal to 0 and subsequent entries equal to 1.