Collective Rydberg excitations of an atomic gas confined in a ring lattice

B. Olmos, R. González-Férez, and I. Lesanovsky
Phys. Rev. A 79, 043419 – Published 24 April 2009

Abstract

We study the excitation dynamics of Rydberg atoms in a one-dimensional lattice with periodic boundary conditions where the atomic Rydberg states are resonantly excited from the electronic ground state. Our description of the corresponding dynamics is numerically exact within the perfect blockade regime, i.e., no two atoms in a given range can be excited. The time evolution of the mean Rydberg density, density-density correlations, as well as entanglement properties is analyzed in detail. We demonstrate that the short-time dynamics is universal and dominated by quantum phenomena, while for larger time the characteristics of the lattice become important and the classical features determine the dynamics. The results of the perfect blockade approach are compared to the predictions of an effective Hamiltonian which includes the interaction of two neighboring Rydberg atoms up to the second-order perturbation theory.

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  • Received 29 December 2008

DOI:https://doi.org/10.1103/PhysRevA.79.043419

©2009 American Physical Society

Authors & Affiliations

B. Olmos1,*, R. González-Férez1,†, and I. Lesanovsky2,3,‡

  • 1Departamento de Física Atómica, Molecular y Nuclear and Instituto “Carlos I” de Física Teórica y Computacional, Universidad de Granada, E-18071 Granada, Spain
  • 2Institute of Theoretical Physics, University of Innsbruck and Institute for Quantum Optics and Quantum Information, Austrian Academy of Sciences, Innsbruck A-6020, Austria
  • 3School of Physics and Astronomy, The University of Nottingham, Nottingham NG7 2RD, United Kingdom

  • *bolmos@ugr.es
  • rogonzal@ugr.es
  • igor.lesanovsky@nottingham.ac.uk

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Issue

Vol. 79, Iss. 4 — April 2009

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