00:01
Okay, so consider a finite dimensional in a product space v and a linear operator t on v.
00:10
We will use the notation w to denote a t -invariant subspace.
00:22
Well, what does it mean for a subspace to be t -invariant? it just means that for any element little w within that subspace, when you apply that transformation t to it, it remains within that subspace.
00:36
That's why it's called t -invariant.
00:39
So now the result that we want to show is that we consider w -p, which is the set that is orthogonal to w, then it corresponds to the t -star, or tier joint, invariant subspace.
00:58
Okay, so how would we go about showing something like this? well, it's basically going to turn out several lines of inner product manipulation.
01:08
So let you be something inside w -prp, and let w be something inside big w...