Understanding the Identity Operator in 2-Qubit Quantum Systems

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SUMMARY

The discussion centers on the identity operator in 2-qubit quantum systems, specifically the unitary transformation \(\mathbf{U}_f\) defined as \(\mathbf{U}_f(\left| x\right>\left| y\right>) = \left| x\right>\left| y \oplus f(x)\right>\), where \(f\) is a 1-bit function. It is established that when \(f(0) = 0\) and \(f(1) = 0\), the transformation simplifies to the identity operator \(\mathbf{1}\). The participants confirm that \(\left| x\right>\left| y\right>\) represents a tensor product, although they acknowledge the informal notation used in discussions.

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Dragonfall
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Suppose \mathbf{U}_f(\left| x\right>\left| y\right> )=\left| x\right>\left| y\oplus f(x)\right> denotes the unitary transformation corresponding to some 1-bit function f.

I'm guessing here that x is the input register, and y the output register.

Now suppose f(0)=0 and f(1)=0.

How is it that \mathbf{U}_f=\mathbf{1} the 2-Qbit unit operator?
 
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In general, is \left| x\right>\left| y\right> a tensor product?
 
don't know about your first question but in general \left| x\right>\left| y\right>
means tensor product, we are just too lazy to write it.
 
It might be better to post this under "quantum mechanics".
 

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