Abstract

Adiabatic techniques can be used to control quantum states with high fidelity while exercising limited control over the parameters of a system. However, because these techniques are slow compared to other timescales in the system, they are usually not suitable for creating highly unstable states or performing time-critical processes. Both of these situations arise in quantum information processing, where entangled states may be isolated from the environment only for a short time and where quantum computers require high-fidelity operations to be performed quickly. Recently it has been shown that techniques like optimal control and shortcuts to adiabaticity can be used to prepare quantum states non-adiabatically with high fidelity. Here we present two examples of how these techniques can be used to create maximally entangled many-body NOON states in one-dimensional Tonks–Girardeau gases.

Highlights

  • Macroscopic superposition states, such as the maximally entangled |N, 0 + |0, N (NOON) state, are of great interest for fundamental studies of quantum mechanics and for applications in quantum information and quantum metrology

  • A theoretical proposal for an experimentally realistic setup for creating NOON states for a large number of ultracold atoms was recently presented by Hallwood et al [3], who considered a gas of strongly interacting bosons in a one-dimensional ring

  • This leaves the system in a NOON state without the need for a potential barrier, which is different from the infidelity, 1 − F infidelity, 1 − F

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Summary

Introduction

Macroscopic superposition states, such as the maximally entangled |N, 0 + |0, N (NOON) state, are of great interest for fundamental studies of quantum mechanics and for applications in quantum information and quantum metrology. A theoretical proposal for an experimentally realistic setup for creating NOON states for a large number of ultracold atoms was recently presented by Hallwood et al [3], who considered a gas of strongly interacting bosons in a one-dimensional ring In this proposed system, states with different angular momentum may become coupled by breaking the rotational symmetry, and the authors have shown how to accelerate the atoms into a superposition state of rotating and non-rotating components. The paper is organised as follows: In Section 2 we begin briefly review the ring system of strongly correlated ultracold atoms proposed by Hallwood et al [3]

Creating a NOON state on a ring
Optimal Control
Optimising over the rotational velocity
Optimising over the barrier height
Optimising over rotational velocity and barrier height
Tonks–Girardeau gas acceleration
Shortcuts to adiabaticity
Lewis–Riesenfeld invariants
Shortcut for the acceleration
Harmonic and sinusoidal potentials
Single particle acceleration
Conclusion
Full Text
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