Commutation relations trouble (basic)

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    Commutation Relations
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Discussion Overview

The discussion revolves around the commutation relations of quantum mechanical operators, specifically addressing the implications of these relations on their eigenstates. Participants explore the conditions under which operators commute and the nature of their eigenstates, referencing concepts from quantum mechanics literature.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant notes that if two operators commute, they share the same set of eigenstates, but questions this in the context of angular momentum operators where certain pairs do not commute.
  • Another participant explains that while simultaneous eigenstates of certain operators can be constructed, not every eigenstate of one operator is necessarily an eigenstate of another, particularly when considering superpositions.
  • A later reply suggests a rephrasing of the initial statement about commuting operators and their eigenstates, emphasizing that while some combinations can yield eigenstates of both operators, this does not apply universally to all eigenstates.
  • Technical details regarding the conditions for operators to commute are introduced, highlighting the mathematical framework behind the discussion.

Areas of Agreement / Disagreement

Participants express differing interpretations of the implications of commutation relations on eigenstates, indicating that there is no consensus on the precise nature of these relationships. The discussion remains unresolved regarding the strength and accuracy of the statements about eigenstates.

Contextual Notes

Participants highlight limitations in understanding the relationships between eigenstates and the conditions under which operators commute, indicating a need for careful consideration of definitions and assumptions in quantum mechanics.

quasar987
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I am reading the first chapter of Sakurai's Modern QM and from pages 30 and 32 respectively, I understand that

(i) If [A,B]=0, then they share the same set of eigenstates.

(ii) Conversely, if two operators have the same eigenstates, then they commute.

But we know that [L^2,L_z]=0, [L^2,L_x]=0 and [L_z,L_x]\neq 0.

From the first equality, and (i) I gather that L² and L_z have the same eigenkets. From (i) and the second equality, I get that L² and L_x have the same eigenkets. So L_z and L_x have the same eigenkets. Hence, by (ii), they commute, which contradicts [L_z,L_x]\neq 0.

Where did I go wrong??
 
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Hi quasar,

Consider the states | \ell, \,m_z \rangle which are the usual simultaneous eigenstates of L^2 and L_z. To understand your problem, imagine taking superpositions of these states with the same \ell but different m_z values. For example, the state | 1/2,\, 1/2 \rangle + | 1/2, \,-1/2 \rangle is such a superpostion; an equal superposition of spin up and spin down. This state is not an eigenstate of L_z (two different m_z values), but it is still an eigenstate of L^2. Thus while it is certainly possible to choose simultaneous eigenstates of L_z and L^2, it is definitely not true that every eigenstate of L^2 is an eigenstate of L_z. In fact, the state I just constructed is nothing other than the spin up eigenstate of L_x. That is, it is a simultaneous eigenstate of L^2 and L_x rather than L^2 and L_z. So you see, among all the states with the same value of \ell, there is a nontrivial freedom to construct states that are eigenstates of L_z or L_x. Finally, the fact that L_z and L_x don't commute simple means that you won't be able find to find linear combinations which are eigenstates of L_z and L_x.

Hope this helps!
 
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Ah, so I misinterpreted (i). Would a true statement be that if [A,B]=0, then the eigenkets of either one of A or B are eigenkets for the other.

Correct? Can it be made stronger?
 
quasar987 said:
Ah, so I misinterpreted (i). Would a true statement be that if [A,B]=0, then the eigenkets of either one of A or B are eigenkets for the other.

The crucial point is that the above statement is definitely not true; eigenstates of A are in no way guaranteed to be eigenstates of B. The guarantee you do have is much weaker. What it says is that if you make a list of linearly independent eigenstates of A with the same eigenvalue, then you can always make from this list states which are also eigenstates of B (provided A and B commute). Again, it does not mean that every state on your list is automatically an eigenstate of B, only that you can find some combinations which are.
 
Thank you!
 
Technically, if A:D(A)\rightarrow \mbox{Im}(A) ,A:D(B)\rightarrow \mbox{Im}(B) AND D(A) \cap D(B) \neq \emptyset, then

AB-BA=0 \Leftrightarrow A(B\psi)=B(A\psi), \forall \in \psi D(A) \cap D(B) \ \mbox{and} \ B\psi \in D(A) , A\psi \in D(B).

Daniel.
 

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