Quantum state preparation of spin eigenstates including the Dicke states with generalized all-coupled interaction in a spintronic quantum computing architecture

TL;DR

This paper presents a deterministic method for preparing arbitrary spin eigenstates, including Dicke states, in a spintronic quantum architecture using uniform all-to-all coupling and iterative spin pumping, improving efficiency over previous methods.

Contribution

It introduces a new algorithm for efficiently preparing complex entangled states like Dicke states with linear or logarithmic circuit depth in a spintronic system.

Findings

Deterministic preparation of Dicke states in linear steps.

Logarithmic circuit depth for W state preparation.

Effective use of all-to-all exchange coupling in spintronic architecture.

Abstract

There has been an extensive development in the use of multi-partite entanglement as a resource for various quantum information processing tasks. In this paper we focus on preparing arbitrary spin eigenstates whose subset contain important entangled resources like Dicke states as well as some other sub-radiant states that are difficult to prepare. Leveraging on the symmetry of these states we consider uniform pairwise exchange coupling between every pair of qubits. Starting from a product state of a given spin eigenstate with a single qubit state, another spin eigenstate can be prepared using simple time evolutions. This expansion paves a deterministic approach to prepare arbitrary Dicke states in linear steps. We discuss an improvement in this cost building up on a previous work for W states deterministic preparation in logarithmic circuit depth. The modified algorithm requires several iterations of pumping spin angular momentum into the system and is akin to the amplitude amplification in Grover search. As a use case to demonstrate the proposed scheme, we choose a system of non-interacting static spin qubits connected to a ferromagnetic reservoir. The flying qubits emerging from the reservoir locally interact with static qubits successively, mediating an in-direct exchange interaction between all the pairs.