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 is
With 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 require
A 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 vectors
The desired outputs have the symmetric expressions
Choose the actual outputs to be
They are normalized and satisfy
Consequently 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 basis
Choose two further orthonormal vectors perpendicular to ,
Then
maps 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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