Rydberg quantum controlled-phase gate with one control and multiple target qubits
Su S L
       

(color online) Energy levels, laser couplings, and the RRIs of (a) the control atom and (b) the target atoms used to construct the n-qubit controlled-phase gate. |R〉, |r〉 |a〉, and |b〉 denote the Rydberg states. |R1|rk → |b1|ak with defect δ2 and strength V2, and |r1|Rk → |a1|bk with defect δ1 and strength V1. VRr is the strength of the dipole–dipole interaction between the control and target atoms. Vrr is the strength of the vdW interaction among the target atoms. The scheme requires VRrVrr,[69] which can be achieved by using Förster resonances and choosing suitable and n.[73] The Rydberg state |a〉- and |b〉-induced transitions, as well as the vdW interactions Vrr give rise to the transition errors. Ω1(k) is the Rabi frequency of the transitions |1〉 ↔ |R1 (|1〉 ↔ |rk) of control atom 1 (target atom k). |0〉 and |1〉 constitute the computation subspace.