In the book chapter6.2, it says when A and B both diagonalizable, AB=BA is true if and only if they have the same eigenvectors. It's easy to obtain that AB=BA,but how to prove vise versa??
The statement does not depend of basis choice, so let's consider the basis, consisting from eigenvectors of A. Matrix presentation of A is diagonal in that basis. AB=BA implies that matrix presentation of B is a diagonal matrix, which means that basis vectors are eigenvectors of B.
Let's say if A has totally different eigenvalues, ΛB=BΛ (Λ , the diagonal matrix of A) deduces that B is also diagonal, very well. What if Λ has the same eigenvalue, I don't think B is diagonal deduced from ΛB=BΛ. Also, AB=BA equal to ΛB=BΛ? IF A=SΛS^(-1), then SΛS^(-1)B=BSΛS^(-1), how I get ΛB=BΛ?
I like your question. Generally speaking the statement of your theorem is not true. However, existence of common basis formed by eigenvectors of diagonalizable A and B is equivalent to AB = BA. Consider extreme case when all eigenvalues of A are the same. Then any vector of n-dimensional space Rn is an eigenvector of A. In that case the statement that A and B have common basis formed by eigenvectors is trivial. I will show proof of the general case later today.
Your last question: "Also, AB=BA equal to ΛB=BΛ? IF A=SΛS^(-1), then SΛS^(-1)B=BSΛS^(-1), how I get ΛB=BΛ?" Answer: When A = S*DIAG*S^(-1) then B transforms to B' = S*B*S^(-1), so AB=BA => DIAG*B' = B'*DIAG. In other words, property AB = BA does not depend from choice of the basis.
Thanks for your patient answer! There's still doubts..but I'll wait and see your proof of general case first.
General case. 1. There exists basis formed by eigenvectors of A, since A is diagonalizable. 2. Sort the basis vectors by ascending order of corresponding eigenvalues. In that basis: a) Matrix representation of A is a diagonal matrix DIAG. b) Matrix representation of B is cellular-diagonal matrix CELL, as follows from equation AB=BA. 3. Since B-cells outside of main diagonal are zeroes, each group of basis vectors, corresponding the same eigenvalue of A, spans a B-invariant subspace. 4. Restriction of B on that subspace is also diagonalizable. 5. There exists a basis of that subspace formed by eigenvectors of B. 6. All base vectors of this basis are eigenvectors of A, since any vector of this subspace is an eigenvector of A ( as in extreme case above). 7. Union of all such base systems forms common basis in Rn, consisting of common eigenvectors of A and B.
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