Put . Factoring the target operator giveswhereas . Their difference is a relative phase on the first qubit, not one overall global phase.
For an explicit witness, choose the product input , with any normalized . The first-qubit outputs are respectively and . A Hadamard basis measurement returns with probabilitiesThese differ because is not a multiple of . The two unitary operators implement different quantum channels. The global phase of the conditional target operation has become a physically observable phase on its control.
No: is not an entangling gate. Its factorization gives, for every product input,which remains a product state. More generally, a convex mixture of product density matrices remains separable under these local unitary operators. Thus being distinguishable from does not require creating entanglement. The first qubit undergoes a genuine local phase gate, while the target undergoes the same in both branches.
Articles by others on the same topic
There are currently no matching articles.