Does Commuting with Hamiltonian Ensure Observables' Commutator is Constant?

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Homework Help Overview

The discussion revolves around the proof that if two observables, Q1 and Q2, are constants of motion for a Hamiltonian H, then their commutator [Q1, Q2] is also a constant of motion. Participants are exploring the implications of the commutation relations between these operators and the Hamiltonian.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to establish the proof by manipulating the commutation relations and questions whether their interpretation of the problem is correct. Some participants question the necessity of assuming that Q1 and Q2 commute, suggesting that the proof can be approached without this assumption.

Discussion Status

The discussion is active, with participants providing feedback on the original poster's reasoning and suggesting alternative approaches. There is an emphasis on clarifying assumptions and the validity of the steps taken in the proof.

Contextual Notes

Participants note that the problem does not explicitly state that Q1 and Q2 commute, which raises questions about the assumptions being made in the proof. This highlights the importance of carefully considering the conditions under which the proof is being conducted.

syang9
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[SOLVED] commutation of observables

Homework Statement



Prove: If the observables (operators) Q1 and Q2 are both constant of the motion for some Hamiltonian H, then the commutator [Q1, Q2] is also a constant of the motion.

okay, first question.. am i being asked to prove that [[Q1, Q2], H] = 0? If so, then consider the following.. if not.. well, that sucks.

Given that they are 'constant of the motion', that means they commute with the Hamiltonian, right..? So that gives us

<br /> \[[H,Q_1 ] = 0\]<br /> \[[H,Q_2 ] = 0\]<br />

Then maybe I can say..

<br /> \[HQ_1 - Q_1 H = HQ_2 - Q_2 H\]<br />

I can multiply through the left side by Q2 to get

<br /> \[Q_2 HQ_1 - Q_2 Q_1 H = 0\]<br />

Since Q2 is an observable, it's a hermitan operator, which allows me to move Q2 to the other side in that first term, like this..

<br /> \[HQ_1 Q_2 - Q_2 Q_1 H = 0\]<br />

which is equivalent to saying

<br /> \[[H,Q_1 Q_2 ] = 0\]<br />

Going back to what I was asked to prove (hopefully), which was:
<br /> \[[[Q_1 Q_2 - Q_2 Q_1 ],H] = 0\]<br />

Expanding that out, we have
<br /> \[Q_1 Q_2 H - Q_2 Q_1 H - HQ_1 Q_2 + HQ_2 Q_1 = 0\]<br />

but I've already proved that [H, Q1Q2] = 0, so we can rewrite this as:

<br /> <br /> \[<br /> ({Q_1 Q_2 H - HQ_1 Q_2 }) - ({Q_2 Q_1 H - HQ_2 Q_1 }) = 0<br /> \]<br /> <br />

which we know is equivalent to
<br /> \[[H,Q_1 Q_2 ] - [H,Q_1 Q_2 ] = 0\]<br />

Since [H, Q1Q2] = 0, both sides are equal to zero, and the proof is... complete? Have I done anything wrong?
 
Last edited:
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syang9 said:

Homework Statement


Since Q2 is an observable, it's a hermitan operator, which allows me to move Q2 to the other side in that first term, like this..

<br /> \[HQ_1 Q_2 - Q_2 Q_1 H = 0\]<br />

There might be a breakdown of logic here. It seems to me that you are also assuming that Q1 and Q2 commute, which is an unnecessary assumption. I think the proof should be easier than you are making it.
 
Why is it unnecessary? Is what I've said incorrect?
 
It is only incorrect if Q1 and Q2 don't commute. In general, they don't have to for the statement that you need to prove to be correct.
You can only move the Q2 through the Q1 (toward the right) if they commute. But nothing in the problem says that you should assume they commute. In fact, you can prove what you need to without this assumption.
 
syang9 said:
Why is it unnecessary? Is what I've said incorrect?

Like Pacopag said, you are assuming that Q1 Q2 = Q2 Q1 which is not necessarily the case.

It's easy. Simply expand [[Q1,Q2],H] completely. Then use that fact that you can move H though Q1 and Q2.
 

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