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Randomized Benchmarking with Non-Markovian Noise and Realistic Finite-Time Gates
Phys. Rev. Lett. 135, 070601 – Published 14 August, 2025
DOI: https://doi.org/10.1103/tmfd-qc5q
Abstract
We analyze the impact of non-Markovian classical noise on single-qubit randomized benchmarking experiments, in a manner that explicitly models the realization of each gate via realistic finite-duration pulses. Our new framework exploits the random nature of each gate sequence to derive expressions for the full survival probability decay curve which are nonperturbative in the noise strength. In the presence of non-Markovian noise, our approach shows that the decay curve can exhibit a strong dependence on the gate implementation method, with regimes of both exponential and power law decays. We discuss how these effects can complicate the interpretation of a randomized benchmarking experiment, but also how to leverage them to probe non-Markovianity.
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References (35)
- E. Knill, D. Leibfried, R. Reichle, J. Britton, R. B. Blakestad, J. D. Jost, C. Langer, R. Ozeri, S. Seidelin, and D. J. Wineland, Phys. Rev. A 77, 012307 (2008).
- E. Magesan, J. M. Gambetta, and J. Emerson, Phys. Rev. Lett. 106, 180504 (2011).
- E. Magesan, J. M. Gambetta, and J. Emerson, Phys. Rev. A 85, 042311 (2012).
- J. Helsen, I. Roth, E. Onorati, A. H. Werner, and J. Eisert, PRX Quantum 3, 020357 (2022).
- A. Hashim, L. B. Nguyen, N. Goss, B. Marinelli, R. K. Naik, T. Chistolini, J. Hines, J. P. Marceaux, Y. Kim, P. Gokhale, T. Tomesh, S. Chen, L. Jiang, S. Ferracin, K. Rudinger, T. Proctor, K. C. Young, R. Blume-Kohout, and I. Siddiqi, arXiv:2408.12064.
- Y. Kim, L. C. G. Govia, A. Dane, E. van den Berg, D. M. Zajac, B. Mitchell, Y. Liu, K. Balakrishnan, G. Keefe, A. Stabile, E. Pritchett, J. Stehlik, and A. Kandala, arXiv:2407.02467.
- K. X. Wei, E. Pritchett, D. M. Zajac, D. C. McKay, and S. Merkel, Phys. Rev. Appl. 21, 024018 (2024).
- E. Paladino, Y. M. Galperin, G. Falci, and B. L. Altshuler, Rev. Mod. Phys. 86, 361 (2014).
- M. Veldhorst, J. C. C. Hwang, C. H. Yang, A. W. Leenstra, B. de Ronde, J. P. Dehollain, J. T. Muhonen, F. E. Hudson, K. M. Itoh, A. Morello, and A. S. Dzurak, Nat. Nanotechnol. 9, 981 (2014).
- C. A. Ryan, M. Laforest, and R. Laflamme, New J. Phys. 11, 013034 (2009).
- P. Figueroa-Romero, K. Modi, and M.-H. Hsieh, Quantum 6, 868 (2022).
- B. H. Fong and S. T. Merkel, arXiv:1703.09747.
- P. Figueroa-Romero, K. Modi, R. J. Harris, T. M. Stace, and M.-H. Hsieh, PRX Quantum 2, 040351 (2021).
- M. A. Fogarty, M. Veldhorst, R. Harper, C. H. Yang, S. D. Bartlett, S. T. Flammia, and A. S. Dzurak, Phys. Rev. A 92, 022326 (2015).
- H. Ball, T. M. Stace, S. T. Flammia, and M. J. Biercuk, Phys. Rev. A 93, 022303 (2016).
- C. L. Edmunds, C. Hempel, R. J. Harris, V. Frey, T. M. Stace, and M. J. Biercuk, Phys. Rev. Res. 2, 013156 (2020).
- X. Zhang, Z. Wu, G. A. L. White, Z. Xiang, S. Hu, Z. Peng, Y. Liu, D. Zheng, X. Fu, A. Huang, D. Poletti, K. Modi, J. Wu, M. Deng, and C. Guo, Randomised benchmarking for characterizing and forecasting correlated processes (2023) [arXiv:2312.06062].
- P. Groszkowski, A. Seif, J. Koch, and A. A. Clerk, Quantum 7, 972 (2023).
- N. G. Van Kampen, Physica (Amsterdam) 74, 215 (1974).
- N. G. Van Kampen, Physica (Amsterdam) 74, 239 (1974).
- T. Proctor, K. Rudinger, K. Young, M. Sarovar, and R. Blume-Kohout, Phys. Rev. Lett. 119, 130502 (2017).
- J. J. Wallman and J. Emerson, Phys. Rev. A 94, 052325 (2016).
- See Supplemental Material at http://link.aps.org/supplemental/10.1103/tmfd-qc5q [5,18–20,22,24–27] graining approximation and extension to other systems involving random gate sequences.
- R. F. Fox, J. Math. Phys. (N.Y.) 17, 1148 (1976).
- R. Kubo, J. Phys. Soc. Jpn. 17, 1100 (1962).
- A. Winick, J. J. Wallman, D. Dahlen, I. Hincks, E. Ospadov, and J. Emerson, arXiv:2212.07500.
- A. A. Mele, Quantum 8, 1340 (2024).
- K. Serniak, M. Hays, G. de Lange, S. Diamond, S. Shankar, L. D. Burkhart, L. Frunzio, M. Houzet, and M. H. Devoret, Phys. Rev. Lett. 121, 157701 (2018).
- L. Viola and E. Knill, Phys. Rev. Lett. 94, 060502 (2005).
This is a consequence of our assumption that the initial state of the qubit is uncorrelated with the noise.
- Y. Zhang and M. I. Dykman, Phys. Rev. B 92, 165419 (2015).
- J. M. Epstein, A. W. Cross, E. Magesan, and J. M. Gambetta, Phys. Rev. A 89, 062321 (2014).
This crossover between two kinds of decay is reminiscent of (but distinct from) the findings in Ref. [14], where RB decay was described by a sum of two exponential terms.
- A. Erhard, J. J. Wallman, L. Postler, M. Meth, R. Stricker, E. A. Martinez, P. Schindler, T. Monz, J. Emerson, and R. Blatt, Nat. Commun. 10, 5347 (2019).
- https://www.energy.gov/doe-public-access-plan