Understanding the Use of Controlled Not Gates in Quantum Computing

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SUMMARY

The discussion centers on the application of the controlled NOT gate, denoted as \hat{U}_{CNOT}(\theta), in quantum computing and its interaction with the single-bit rotation operator \hat{Z}_A(\theta). The operator \hat{U}_{CNOT}(\theta) is defined as \exp{(-i \theta \hat{U}_{CNOT})}, and when applied to a state, it introduces a relative phase complication. To mitigate this, the author suggests using \hat{Z}_A(\theta) \hat{U}_{CNOT}(\theta) to eliminate the extra relative phase, but the user expresses confusion over how this interaction resolves the phase issue. The article referenced for deeper understanding is available at http://arxiv.org/abs/quant-ph/0108132.

PREREQUISITES
  • Understanding of quantum operators, specifically \hat{U}_{CNOT} and \hat{Z}_A.
  • Familiarity with quantum state notation, including Dirac notation (|0⟩, |1⟩).
  • Basic knowledge of quantum mechanics principles, particularly phase relations.
  • Experience with mathematical operations involving matrices, such as \hat{\sigma}_x.
NEXT STEPS
  • Study the mathematical properties of the controlled NOT gate, \hat{U}_{CNOT}.
  • Learn about the effects of single-bit rotation operators like \hat{Z}_A on quantum states.
  • Explore the implications of relative phase in quantum mechanics and its impact on quantum computations.
  • Review the article at http://arxiv.org/abs/quant-ph/0108132 for further insights into the calculations involving \hat{Z}_A and \hat{U}_{CNOT}.
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Quantum computing enthusiasts, researchers in quantum mechanics, and students seeking to understand the complexities of quantum gate operations and their mathematical implications.

ShayanJ
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In an article I'm reading, the author defines an operator as below:
<br /> \hat{U}_{CNOT}(\theta)=\exp{(-i \theta \hat{U}_{CNOT})}=\hat{1} \cos{\theta}-i \hat{U}_{CNOT} \sin{\theta}<br />
Where \hat{U}_{CNOT} is the controlled not gate(http://en.wikipedia.org/wiki/Controlled_NOT_gate).
Then the operator is applied to a state of the form (\alpha |0\rangle+\beta|1\rangle) \otimes |\psi\rangle and the resulting state is:
<br /> (\alpha e^{-i \theta} |0\rangle+\beta \cos{\theta} |1\rangle)\otimes |\psi\rangle-i \beta \sin{\theta} |1\rangle \otimes (\hat{\sigma}_x |\psi\rangle)<br />
where \hat{\sigma}_x=\begin{pmatrix}<br /> 0&amp;1\\<br /> 1&amp;0<br /> \end{pmatrix}
Then the author says:
The relative phase e^{i \theta} between |0\rangle and |1\rangle is a complication in the calculations that will follow.To avoid this problem, instead of \hat{U}_{CNOT}(\theta),we will use interactions of the form \hat{Z}_A(\theta) \hat{U}_{CNOT}(\theta),where\hat{Z}_A(\theta)=(\exp{(i \hat{\sigma}_z \theta/2)}\otimes \hat{1})...The single-bit rotation exactly undoes the extra relative phase produced by \hat{U}_{CNOT},while changing nothing else.
Now my problem is that I can't understand how that happens. I don't know how to work with \hat{Z}_A(\theta)\hat{U}_{CNOT}(\theta).I'll appreciate any suggestion.
Thanks
 
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In an article I'm reading
Meaningless without citations.
Which article - where - when - who is the author?

But I think this is just a handy notation to remove a nasty bit of math.
Z does what it is defined to do. The author is only using it by defining it.
See what happens next.
 
Yeah,I wasn't clear enough,sorry.
This is the link to the article:http://arxiv.org/abs/quant-ph/0108132
But the part that I mentioned,doesn't need much knowledge about the other parts of the article.
My problem is that when I apply \hat{Z}_A(\theta) to \hat{U}_{CNOT}(\theta)(\alpha |0 \rangle +\beta|1\rangle)\otimes |\psi \rangle,there is still a relative phase between |0\rangle and |1\rangle which leads me to think I'm missing sth.
Also I can't get help from the article itself,because it doesn't contain calculations that I want.
 
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