Logics of Quantum Computation with Quantum Simulable Operators
Martinvaldo Konig
Abstract
Abstract In quantum computational logics meaning of sentences are repre-sented by quantum information quantities. Any n-qubit sequence is identified with a unit vector of the tensor product of the complex Hilbert space ⊗nC2. Let us split the set of the vectors of its computational basis in the two sets: Bn1: = {i: ‖ i À= | x1,.., xn 〉 and xn = 1}; Bn0: = {i: ‖ i À= | x1,.., xn 〉 and xn = 0}. Any unit vector | ψ 〉 can be expressed in the form: | ψ 〉 = ∑i∈B0 ai ‖ iÀ +∑j∈B1 bj ‖ j À where by the Born rule,∑ i∈B0 | ai |2 + j∈B1 | bj |2 = 1 A key role in the definition of semantics is played by the probability-value of | ψ〉, defined as follows: p( | ψ〉): = ∑j∈B1 | bj |2 Moreover a function g: [0, 1]2 7 → [0, 1] is said quantum simulable iff ∃n ≥ 1, a unitary operator Ug: ⊗n+2C2 7 → ⊗n+2C2 and a quregister | χ 〉 ∈ ⊗nC2 such