Home | About Journal | Web Links | E-mail Alerts | RSS RSS Icon | Browse
Previous Article Next Article

Vacuum Degeneracy of a Circuit QED System in the Ultrastrong Coupling Regime

Source: Phys. Rev. Lett. 104, 023601 (2010); doi:10.1103/PhysRevLett.104.023601

Published 15 January 2010

PACS
  • 64.70.Tg
    Quantum phase transitions
  • 03.67.Pp
    Quantum error correction and other methods for protection against decoherence
  • 42.50.-p
    Quantum optics
  • 85.25.-j
    Superconducting devices
  • YEAR: 2010
PUBLICATION DATA
Publisher:
AIP is a member of CrossRef APS
Pierre Nataf and Cristiano Ciuti
Laboratoire Matriaux et Phnomnes Quantiques, Universit Paris Diderot-Paris 7 and CNRS, Btiment Condorcet, 10 rue Alice Domont et Lonie Duquet, 75205 Paris Cedex 13, France
We investigate theoretically the quantum vacuum properties of a chain of N superconducting Josephson atoms inductively coupled to a transmission line resonator. We derive the quantum field Hamiltonian for such a circuit QED system, showing that, due to the type and strength of the interaction, a quantum phase transition can occur with a twice degenerate quantum vacuum above a critical coupling. In the finite-size case, the degeneracy is lifted, with an energy splitting decreasing exponentially with increasing values of g2N2, where g is the dimensionless vacuum Rabi coupling per artificial atom. We determine analytically the ultrastrong coupling asymptotic expression of the two degenerate vacua for an arbitrary number of artificial atoms and of resonator modes. In the ultrastrong coupling regime the degeneracy is protected with respect to random fluctuations of the transition energies of the Josephson elements. ©2010 The American Physical Society
History: Received 23 September 2009; revised 30 November 2009; published 15 January 2010
Permalink: http://link.aps.org/abstract/PRL/v104/e023601
ADVERTISEMENT