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Time evolution of the one-dimensional Jaynes-Cummings-Hubbard Hamiltonian

Source: Phys. Rev. A 80, 043842 (2009); doi:10.1103/PhysRevA.80.043842

Published 30 October 2009

KEYWORDS and PACS
Keywords
PACS
  • 42.50.Pq
    Cavity quantum electrodynamics; micromasers
  • 42.50.Gy
    Effects of atomic coherence on propagation, absorption, and amplification of light
  • 05.60.Gg
    Quantum transport
  • YEAR: 2009
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
M. I. Makin,1 Jared H. Cole,2 Charles D. Hill,1 Andrew D. Greentree,1 and Lloyd C. L. Hollenberg1
1Center for Quantum Computer Technology, School of Physics, The University of Melbourne, Victoria 3010, Australia
2Institut für Theoretische Festkörperphysik and DFG-Center for Functional Nanostructures (CFN), Universität Karlsruhe, Karlsruhe 76128, Germany

The Jaynes-Cummings-Hubbard (JCH) system describes a network of single-mode photonic cavities connected via evanescent coupling. Each cavity contains a single two-level system which can be tuned in resonance with the cavity. Here, we explore the behavior of single excitations (where an excitation can be either photonic or atomic) in the linear JCH system, which describes a coupled cavity waveguide. We use direct, analytic diagonalization of the Hamiltonian to study cases where intercavity coupling is either uniform or varies parabolically along the chain. Both excitations located in a single cavity, as well as one excitation as a Gaussian pulse spread over many cavities, are investigated as initial states. We predict unusual behavior of this system in the time domain, including slower than expected propagation of the excitation and also splitting of the excitation into two distinct pulses, which travel at distinct speeds. In certain limits, we show that the JCH system mimics two Heisenberg spin chains. ©2009 The American Physical Society
History: Received 3 July 2009; published 30 October 2009
Permalink: http://link.aps.org/abstract/PRA/v80/e043842
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