Proof: 3 Reversible evolutions -- Hermitian Conjugate

AI Thread Summary
The discussion focuses on proving that for a qubit undergoing three reversible evolutions represented by unitary matrices A, B, and C, the relationship C = (BA)† must hold to return to the initial state |v>. The proof begins with the equation C(BA)|v> = |v>, leading to the conclusion that C(BA) = I, where I is the identity matrix. Participants emphasize that this must be valid for all possible states |v>, which allows for the cancellation of |v> in the proof. The importance of recognizing that A and B are unitary matrices is also noted, as it underpins the validity of the steps taken. Overall, the proof is deemed successful, provided that the conditions regarding the unitary nature of A and B are respected.
RJLiberator
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Homework Statement


Consider a qubit whihc undergoes a sequence of three reversible evolutions of 3 unitary matrices A, B, and C (in that order). Suppose that no matter what the initial state |v> of the qubit is before the three evolutions, it always comes back to the sam state |v> after the three evolutions.
Show that we must have C=(BA)†

Homework Equations


† = hermitian conjugate

The Attempt at a Solution



The diagram of the reversible evolution allows us to see that the process |v> --> A --> B --> C = |v> results in the equation:

C(BA)|v> = |v>
From here we see that: C(BA) = I (where I is the identity matrix)
We multiple both sides by (BA)†
C(BA)(BA)†=I(BA)†
By definition of unitary we see
C=(BA)†This was quite easy, we see it only took 3-4 steps.

Have I successfully completed this proof? Recall, I needed to show that this works for all possible |v>.
|v> seems irrelevant, however, since it could be 'cancelled' out in the second step.

Success? Or failure?
 
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RJLiberator said:
C(BA)(BA)†=I(BA)†
By definition of unitary we see
C=(BA)†
I would give more details here, as you can only take that A is unitary and B is unitary, not suppose it for BA.
RJLiberator said:
Have I successfully completed this proof? Recall, I needed to show that this works for all possible |v>.
|v> seems irrelevant, however, since it could be 'cancelled' out in the second step.
Again, to give more details: ##C(BA)|v\rangle = |v\rangle \, \forall \, |v\rangle \Rightarrow C(BA) = I##. You can only go from the first to the second line if you say that this has to hold for all states.
 
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I would give more details here, as you can only take that A is unitary and B is unitary, not suppose it for BA.

Absolutely excellent point. I glossed over that.

Again, to give more details: C(BA)|v⟩=|v⟩∀|v⟩⇒C(BA)=I. You can only go from the first to the second line if you say that this has to hold for all states.

Indeed, what you suggest seems to bring more clarity.
 
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