4.6 Article

Dicke-state preparation through global transverse control of Ising-coupled qubits

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PHYSICAL REVIEW A
卷 108, 期 1, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.108.012608

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This paper focuses on the engineering of the two-excitation Dicke state ID32) in a three-qubit system with all-to-all Ising-type qubit-qubit interaction and global transverse control fields. A pulse sequence is proposed, consisting of three instantaneous control pulses and two finite-duration Ising-interaction pulses, based on the concept of the symmetric sector. Numerical analysis is conducted to demonstrate the robustness of the proposed state-preparation scheme to systematic errors. The generalization of this scheme to systems with N > 4 qubits is also discussed.
We consider the problem of engineering the two-excitation Dicke state ID32) in a three-qubit system with all-toall Ising-type qubit-qubit interaction, which is also subject to global transverse (Zeeman-type) control fields. The theoretical underpinning for our envisioned state-preparation scheme, in which I000) is adopted as the initial state of the system, is provided by a Lie-algebraic result that guarantees state-to-state controllability of this system for an arbitrary choice of initial and final states that are invariant with respect to permutations of qubits. This scheme is envisaged in the form of a pulse sequence that involves three instantaneous control pulses, which are equivalent to global qubit rotations, and two Ising-interaction pulses of finite durations between consecutive control pulses. The design of this pulse sequence (whose total duration is T ti 0.95 h over bar /J, where J is the Ising-coupling strength) leans heavily on the concept of the symmetric sector, a four-dimensional, permutationally invariant subspace of the three-qubit Hilbert space. We demonstrate the feasibility of the proposed state-preparation scheme by carrying out a detailed numerical analysis of its robustness to systematic errors, i.e., deviations from the optimal values of the eight parameters that characterize the underlying pulse sequence. Finally, we discuss how our proposed scheme can be generalized for engineering Dicke states in systems with N 4 qubits. For the sake of illustration, we describe the preparation of the two-excitation Dicke state ID42) in a four-qubit system.

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