Proof: 3 Reversible evolutions -- Hermitian Conjugate

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SUMMARY

The discussion centers on proving that for a qubit undergoing three reversible evolutions represented by unitary matrices A, B, and C, the relationship C = (BA)† must hold. The proof is established by demonstrating that the sequence of operations leads to the identity matrix I, confirming that the initial state |v⟩ returns unchanged after the transformations. The participants emphasize the necessity of the unitary property of matrices A and B, and the proof's validity across all possible states |v⟩.

PREREQUISITES
  • Understanding of qubit states and notation, specifically |v⟩.
  • Familiarity with unitary matrices and their properties.
  • Knowledge of Hermitian conjugates, denoted as †.
  • Basic principles of linear algebra as applied to quantum mechanics.
NEXT STEPS
  • Study the properties of unitary matrices in quantum mechanics.
  • Learn about the implications of Hermitian conjugates in quantum state transformations.
  • Explore the concept of reversible quantum operations and their mathematical representations.
  • Investigate the significance of the identity matrix in quantum state evolution.
USEFUL FOR

Quantum physicists, students of quantum mechanics, and anyone interested in the mathematical foundations of quantum computing and reversible transformations.

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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