Solution:
A and B have common set of eigenstates.
For these common eigenstates one has ∆A = ∆B = 0 and hence ∆A ∆B = 0. There is a complete common set of собственныхn eigenfunctions, for which, therefore,
[A, B] ψn = (AB - BA) ψn = (anbn - bnan) ψn = 0.
Proof (⇐). Suppose that ea is an eigenfunction A. Then A (Bψa) = ABψa = BAψa = B aψa =
Bψa. Thus, Bψa is also an eigenfunction of A. Then you can select
(i) If a is nondegenerate, then Bψa ψa, say, Bψa = bψa, which means that isa is also
Own function B.
(ii) If a is degenerate (degeneration of s), consider the part of the Hilbert space that covers
functions ψar (r = 1, ..., s). For a given ψap (eigenfunction A), Bψap can also be
written in terms of ψar. Thus, we have a Hermitian operator B in the subspace
functions ψar. In this subspace, B can be diagonalized, and we can use the eigenvalues b1 ,. bs
as a second label, which leads to a common set of eigenfunctions.
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