Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Nonclassical Advantage in Metrology Established via Quantum Simulations of Hypothetical Closed Timelike Curves

David R. M. Arvidsson-Shukur1, Aidan G. McConnell2,3,4, and Nicole Yunger Halpern5,6

  • 1Hitachi Cambridge Laboratory, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom
  • 2Cavendish Laboratory, Department of Physics, University of Cambridge, Cambridge CB3 0HE, United Kingdom
  • 3Laboratory for X-ray Nanoscience and Technologies, Paul Scherrer Institut, 5232 Villigen, Switzerland
  • 4Department of Physics and Quantum Center, Eidgenössische Technische Hochschule Zürich, CH-8093 Zürich, Switzerland
  • 5Joint Center for Quantum Information and Computer Science, NIST and University of Maryland, College Park, Maryland 20742, USA
  • 6Institute for Physical Science and Technology, University of Maryland, College Park, Maryland 20742, USA

Phys. Rev. Lett. 131, 150202 – Published 12 October, 2023

DOI: https://doi.org/10.1103/PhysRevLett.131.150202

Abstract

We construct a metrology experiment in which the metrologist can sometimes amend the input state by simulating a closed timelike curve, a worldline that travels backward in time. The existence of closed timelike curves is hypothetical. Nevertheless, they can be simulated probabilistically by quantum-teleportation circuits. We leverage such simulations to pinpoint a counterintuitive nonclassical advantage achievable with entanglement. Our experiment echoes a common information-processing task: A metrologist must prepare probes to input into an unknown quantum interaction. The goal is to infer as much information per probe as possible. If the input is optimal, the information gained per probe can exceed any value achievable classically. The problem is that, only after the interaction does the metrologist learn which input would have been optimal. The metrologist can attempt to change the input by effectively teleporting the optimal input back in time, via entanglement manipulation. The effective time travel sometimes fails but ensures that, summed over trials, the metrologist’s winnings are positive. Our Gedankenexperiment demonstrates that entanglement can generate operational advantages forbidden in classical chronology-respecting theories.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (68)

  1. V. Giovannetti, S. Lloyd, and L. Maccone, Nat. Photonics 5, 222 (2011).
  2. W. Salmon, S. Strelchuk, and D. Arvidsson-Shukur, Quantum 7, 998 (2023).
  3. A. N. Jordan, J. Martínez-Rincón, and J. C. Howell, Phys. Rev. X 4, 011031 (2014).
  4. J. Dressel, M. Malik, F. M. Miatto, A. N. Jordan, and R. W. Boyd, Rev. Mod. Phys. 86, 307 (2014).
  5. J. Harris, R. W. Boyd, and J. S. Lundeen, Phys. Rev. Lett. 118, 070802 (2017).
  6. D. R. M. Arvidsson-Shukur, N. Yunger Halpern, H. V. Lepage, A. A. Lasek, C. H. W. Barnes, and S. Lloyd, Nat. Commun. 11, 3775 (2020).
  7. N. Lupu-Gladstein, Y. B. Yilmaz, D. R. M. Arvidsson-Shukur, A. Brodutch, A. O. T. Pang, A. M. Steinberg, and N. Y. Halpern, Phys. Rev. Lett. 128, 220504 (2022).
  8. A. A. Semenov, J. Samelin, C. Boldt, M. Schünemann, C. Reiher, W. Vogel, and B. Hage, arXiv:2303.14246.
  9. J. H. Jenne and D. R. M. Arvidsson-Shukur, arXiv:2104.09520.
  10. M. Scandi, P. Abiuso, J. Surace, and D. D. Santis, arXiv:2304.14984.
  11. S. Pang, J. Dressel, and T. A. Brun, Phys. Rev. Lett. 113, 030401 (2014).
  12. L. Xu, Z. Liu, A. Datta, G. C. Knee, J. S. Lundeen, Y.-q. Lu, and L. Zhang, Phys. Rev. Lett. 125, 080501 (2020).
  13. J. H. Jenne and D. R. M. Arvidsson-Shukur, Phys. Rev. A 106, 042404 (2022).
  14. F. Salvati, W. Salmon, C. H. W. Barnes, and D. R. M. Arvidsson-Shukur, arXiv:2307.08648.
  15. Y. Aharonov, D. Z. Albert, and L. Vaidman, Phys. Rev. Lett. 60, 1351 (1988).
  16. I. M. Duck, P. M. Stevenson, and E. C. G. Sudarshan, Phys. Rev. D 40, 2112 (1989).
  17. O. Hosten and P. Kwiat, Science 319, 787 (2008).
  18. J. Tollaksen, J. Phys. A 40, 9033 (2007).
  19. M. F. Pusey, Phys. Rev. Lett. 113, 200401 (2014).
  20. R. Kunjwal, M. Lostaglio, and M. F. Pusey, Phys. Rev. A 100, 042116 (2019).
  21. Y. Aharonov and L. Vaidman, Time in Quantum Mechanics (Springer, New York, 2008), pp. 399–447.
  22. M. S. Leifer and M. F. Pusey, Proc. R. Soc. A 473, 20160607 (2017).
  23. K. Gödel, Rev. Mod. Phys. 21, 447 (1949).
  24. M. S. Morris, K. S. Thorne, and U. Yurtsever, Phys. Rev. Lett. 61, 1446 (1988).
  25. D. Deutsch, Phys. Rev. D 44, 3197 (1991).
  26. C. H. Bennett, in Proceedings of QUPON (Wien, Vienna, 2005).
  27. G. Svetlichny, Int. J. Theor. Phys. 50, 3903 (2011).
  28. S. Lloyd, L. Maccone, R. Garcia-Patron, V. Giovannetti, Y. Shikano, S. Pirandola, L. A. Rozema, A. Darabi, Y. Soudagar, L. K. Shalm, and A. M. Steinberg, Phys. Rev. Lett. 106, 040403 (2011).
  29. S. Lloyd, L. Maccone, R. Garcia-Patron, V. Giovannetti, and Y. Shikano, Phys. Rev. D 84, 025007 (2011).
  30. J. R. Gott, Phys. Rev. Lett. 66, 1126 (1991).
  31. S. W. Hawking, Phys. Rev. D 46, 603 (1992).
  32. S. Deser, R. Jackiw, and G. ’t Hooft, Phys. Rev. Lett. 68, 267 (1992).
  33. S. M. Carroll, E. Farhi, A. H. Guth, and K. D. Olum, Phys. Rev. D 50, 6190 (1994).
  34. J.-M. A. Allen, Phys. Rev. A 90, 042107 (2014).
  35. T. A. Brun and M. M. Wilde, Found. Phys. 47, 375 (2017).
  36. M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information: 10th Anniversary Edition, 10th ed. (Cambridge University Press, New York, 2011).
  37. C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres, and W. K. Wootters, Phys. Rev. Lett. 70, 1895 (1993).
  38. B. Coecke, arXiv:quant-ph/0402014.
  39. A teleportation scheme that takes all possible outcomes into account, without the receiver’s performing any local operations, transports an unknown qubit exactly as ineffectively as random guessing.

  40. S. L. Braunstein and C. M. Caves, Phys. Rev. Lett. 72, 3439 (1994).
  41. We choose this simple, common two-qubit interaction to align with previous works [19, 20] and to illustrate our metrological advantage. More general interactions imply analogous results, at the expense of more tedious analytics.

  42. J. Combes, C. Ferrie, Z. Jiang, and C. M. Caves, Phys. Rev. A 89, 052117 (2014).
  43. C. Ferrie and J. Combes, Phys. Rev. Lett. 112, 040406 (2014).
  44. D. R. M. Arvidsson-Shukur, J. C. Drori, and N. Y. Halpern, J. Phys. A 54, 284001 (2021).
  45. R. W. Spekkens, Phys. Rev. A 71, 052108 (2005).
  46. M. Lostaglio, Phys. Rev. Lett. 125, 230603 (2020).
  47. Even if our delay’s precise length is chosen artificially, our story cleaves to the real-world principle that metrology tends to involve delays. For example, optimal input states are generally known only once the specifics of the interaction are known [2, 40, 48].

  48. V. Giovannetti, S. Lloyd, and L. Maccone, Phys. Rev. Lett. 96, 010401 (2006).
  49. In general, ⟨i−|i+⟩≠0.

  50. This postselection is onto a copy of the state prepared initially, |Φ+⟩. Therefore, our simulated CTC preserves correlations (between chronology-violating and chronology-respecting systems), as required by the definition of PCTCs.

  51. See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevLett.131.150202 supporting calculations, generalizations, and practical extensions.
  52. M. Barbieri, C. Cinelli, P. Mataloni, and F. De Martini, Phys. Rev. A 72, 052110 (2005).
  53. C. Cinelli, M. Barbieri, R. Perris, P. Mataloni, and F. D. Martini, Phys. Rev. Lett. 95, 240405 (2005).
  54. J. T. Barreiro, N. K. Langford, N. A. Peters, and P. G. Kwiat, Phys. Rev. Lett. 95, 260501 (2005).
  55. G. Vallone, E. Pomarico, P. Mataloni, F. De Martini, and V. Berardi, Phys. Rev. Lett. 98, 180502 (2007).
  56. K. Chen, C.-M. Li, Q. Zhang, Y.-A. Chen, A. Goebel, S. Chen, A. Mair, and J.-W. Pan, Phys. Rev. Lett. 99, 120503 (2007).
  57. M. A. Ciampini, A. Orieux, S. Paesani, F. Sciarrino, G. Corrielli, A. Crespi, R. Ramponi, R. Osellame, and P. Mataloni, Light Sci. Appl. 5, e16064 (2016).
  58. In principle, also the input state of the probe B could be created at a later time and probabilistically teleported to the beginning of the experiment.

  59. T. A. Brun, Found. Phys. Lett. 16, 245 (2003).
  60. S. Aaronson, arXiv:quant-ph/0412187.
  61. S. Aaronson and J. Watrous, Proc. R. Soc. A 465, 631 (2009).
  62. T. A. Brun, J. Harrington, and M. M. Wilde, Phys. Rev. Lett. 102, 210402 (2009).
  63. T. A. Brun and M. M. Wilde, Found. Phys. 42, 341 (2012).
  64. T. A. Brun, M. M. Wilde, and A. Winter, Phys. Rev. Lett. 111, 190401 (2013).
  65. J. L. Pienaar, T. C. Ralph, and C. R. Myers, Phys. Rev. Lett. 110, 060501 (2013).
  66. J. Bub and A. Stairs, Phys. Rev. A 89, 022311 (2014).
  67. M. Bartkiewicz, A. Grudka, R. Horodecki, J. Łodyga, and J. Wychowaniec, Phys. Rev. A 99, 022304 (2019).
  68. C. Vairogs, V. Katariya, and M. M. Wilde, Phys. Rev. A 105, 052434 (2022).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation