For input , the controlled-NOT gate fixes , which is the ideal two-copy pure state. Thus its global cloning fidelity is . For input , the actual output is the Bell state , whereas the desired output is . Their overlap isWith the given equal input probabilities,These values use the specified squared quantum fidelity for the full output, rather than a one-copy marginal fidelity.
Assume perfect cloning of both specified pure states. Allowing irrelevant output global phases, this would requireA unitary operator preserves inner products, and therefore their magnitudes. But the input overlap and required output overlap have different magnitudes:This contradiction proves that no such two-qubit unitary exists, without assuming the no-cloning theorem.
Construct an economical two-state quantum cloner by moving both actual outputs slightly toward one another relative to the two desired copies. Set and . Their overlap is , so their sum and difference yield the orthonormal vectorsThe desired outputs have the symmetric expressionsChoose the actual outputs to beThey are normalized and satisfyConsequently the prescription , preserves the Gram matrix of the two inputs and defines a linear isometry on their span. The unitary extension of a finite-dimensional isometry gives a unitary operator on the same four-dimensional, two-qubit Hilbert space; no extra workspace is required.
For an explicit full-space construction, define , and the orthonormal basisChoose two further orthonormal vectors perpendicular to ,Thenmaps one orthonormal basis to another and is therefore unitary. Since and , it has exactly the required two outputs.
Finally,Both inputs therefore have the same global cloning fidelity, and so does their average:This proves the requested existence with a two-qubit unitary gate.
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