Commuting Operators: When 2 Operators Don't Commute

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The discussion centers on the commutation relations between quantum operators A, B, and C, specifically addressing the conditions under which they commute or do not commute. It is established that if [A,B]=0 and [A,C]=0, then A, B, and C share a common basis in Hilbert space, particularly when A has degenerate eigenstates. However, if [B,C] is non-zero, B and C do not share a common basis. An example provided is the angular momentum operators, where [{\vec L}^2, L_x]=0 and [{\vec L}^2, L_z]=0, while [L_x, L_y]≠0, illustrating the concept of degeneracy in quantum mechanics.

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Fe-56
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hello...this might look very stupid but I am totally confused...

Let have operators A, B, C. Let [A,B]=[A,C]=0 and [B,C] not 0...

When two operators commute, they have the same base in (Hilbert) space.
So base in A representation is the same as in the B representation and also
the basis in A and C representations are the same.

But if B and C do not commute, their basis are different.



There has to be a fatal error in here:))
thanx:-p
 
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Fe-56 said:
hello...this might look very stupid but I am totally confused...

Let have operators A, B, C. Let [A,B]=[A,C]=0 and [B,C] not 0...

When two operators commute, they have the same base in (Hilbert) space.
So base in A representation is the same as in the B representation and also
the basis in A and C representations are the same.

But if B and C do not commute, their basis are different.



There has to be a fatal error in here:))
thanx:-p

As far as I know, this happens only when there is degeneracy.

Let's say that the eigenstates of A are degenerate. Then if [A,B]=0, it means that the eigenstates of B can be written as some linear combination of the eigenstates of A. If [A,C]= 0, the same thing applies for the eigenstates of C (they can be written as a linear combination of the eigenstates of A).

Consider a set of eigenstates of A all corresponding to the same eigenvalue of A, say A \psi_n(x) = a \psi(x) . Then it will be possible to write some of the eigenstates of B (corresponding possibly to different eigenvalues of B) as some linear combinations of these \psi_n(x). And it will be possible to write some of the eigenstates of C as a different linear combination of the eigenstates of A (still corresponding to the same degenerate eigenvalue a). So A and B share a common set of basis states, A and C share a common basis of states but B and C don't.

An exception is if there is a state for which applying A, B or C all gives zero. Then all three operators may share the same eigenstate even if they don't all commute.


This is what happens, say, with {\vec L}^2 and L_x and L_z for example. We have [ {\vec L}^2,L_x] = [{\vec L}^2,L_z]=0 but [L_x,L_y] \neq 0 .
 
Last edited:
:!)

YES, that's it! :!)

so...there must be degeneracy in all eigenvalues of A, yes?

thankx a lot...



...and this was not any homework, someone replaced it from QT:))
 

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