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
  • Letter
  • Open Access

Implementing a fast unbounded quantum fanout gate using power-law interactions

Andrew Y. Guo1,2,*, Abhinav Deshpande1,2, Su-Kuan Chu1,2, Zachary Eldredge1,2, Przemyslaw Bienias1,2, Dhruv Devulapalli1,2, Yuan Su1,3,4, Andrew M. Childs1,3,4, and Alexey V. Gorshkov1,2

  • 1Joint Center for Quantum Information and Computer Science, NIST/University of Maryland, College Park, Maryland 20742, USA
  • 2Joint Quantum Institute, NIST/University of Maryland, College Park, Maryland 20742, USA
  • 3Department of Computer Science, University of Maryland, College Park, Maryland 20742, USA
  • 4Institute for Advanced Computer Studies, University of Maryland, College Park, Maryland 20742, USA

  • *guoa@umd.edu

Phys. Rev. Research 4, L042016 – Published 27 October, 2022

DOI: https://doi.org/10.1103/PhysRevResearch.4.L042016

Abstract

The standard circuit model for quantum computation presumes the ability to directly perform gates between arbitrary pairs of qubits, which is unlikely to be practical for large-scale experiments. Power-law interactions with strength decaying as 1/rα in the distance r provide an experimentally realizable resource for information processing, whilst still retaining long-range connectivity. We leverage the power of these interactions to implement a fast quantum fanout gate with an arbitrary number of targets. Our implementation allows the quantum Fourier transform (QFT) and Shor's algorithm to be performed on a D-dimensional lattice of qubits in time that scales (poly)logarithmically in the number of qubits, using interactions with α≤2D. As a corollary, we show that power-law systems with α≤2D are difficult to simulate classically even for short times, under a standard assumption that factoring is classically intractable. Complementarily, we develop a technique to give a general lower bound—linear in the size of the system—on the time required to implement the QFT and the fanout gate in systems that are constrained by a linear light cone. This allows us to prove an asymptotically tighter lower bound for long-range systems than was possible with previously available techniques.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (56)

  1. J. Preskill, Quantum computing in the NISQ era and beyond, Quantum 2, 79 (2018).
  2. E. Bernstein and U. Vazirani, Quantum complexity theory, in Proceedings of the Twenty-Fifth Annual ACM Symposium on Theory of Computing - STOC '93 (ACM Press, San Diego, 1993), pp. 11–20
  3. R. Raussendorf and H. J. Briegel, A One-Way Quantum Computer, Phys. Rev. Lett. 86, 5188 (2001).
  4. R. Raussendorf, D. E. Browne, and H. J. Briegel, Measurement-based quantum computation on cluster states, Phys. Rev. A 68, 022312 (2003).
  5. P. Hoyer and R. Spalek, Quantum fanout is powerful, Theory of Comput. 1, 81 (2005).
  6. P. W. Shor, Polynomial-time algorithms for prime factorization and discrete logarithms on a quantum somputer, SIAM J. Comput. 26, 1484 (1997).
  7. While the rate-limiting step for factoring is actually modular exponentiation, it is possible to implement this subroutine in logarithmic quantum depth with a polynomial number of classical gates as a pre-computation step, using a standard universal gate set for quantum computing [39]. Using the unbounded fanout gate, the quantum circuit for modular exponentiation can be reduced to constant depth as well [5].
  8. In this Letter, we use the following standard asymptotic notations: the “big-O” notation f(x)=O(g(x)) indicates the existence of constants c and N such that 0≤f(x)≤cg(x) for all x≥N; the “big-Ω” notation f(x)=Ω(g(x)) indicates that g(x)=O(f(x)); the “big-Θ” notation f(x)=Θ(g(x)) when both f(x)=O(g(x)) and f(x)=Ω(g(x)); finally, the “little-o” notation f(x)=o(g(x)) indicates that limx→∞f(x)/g(x)=0. Additionally, we use poly(n) to refer to computational resources that are polynomial in n.
  9. A. Broadbent and E. Kashefi, Parallelizing quantum circuits, Theor. Comput. Sci. 410, 2489 (2009).
  10. S. A. Fenner, Implementing the fanout gate by a Hamiltonian, arXiv:quant-ph/0309163.
  11. S. A. Fenner and Y. Zhang, Implementing fanout, parity, and Mod gates via spin exchange interactions, arXiv:quant-ph/0407125.
  12. C. Monroe, R. Raussendorf, A. Ruthven, K. R. Brown, P. Maunz, L.-M. Duan, and J. Kim, Large-scale modular quantum-computer architecture with atomic memory and photonic interconnects, Phys. Rev. A 89, 022317 (2014).
  13. N. M. Linke, D. Maslov, M. Roetteler, S. Debnath, C. Figgatt, K. A. Landsman, K. Wright, and C. Monroe, Experimental comparison of two quantum computing architectures, Proc. Natl. Acad. Sci. USA 114, 3305 (2017).
  14. A. Bapat, Z. Eldredge, J. R. Garrison, A. Deshpande, F. T. Chong, and A. V. Gorshkov, Unitary entanglement construction in hierarchical networks, Phys. Rev. A 98, 062328 (2018).
  15. A. M. Childs, E. Schoute, and C. M. Unsal, Circuit Transformations for Quantum Architectures, in 14th Conference on the Theory of Quantum Computation, Communication and Cryptography (TQC 2019) ( Dagstuhl, Germany, 2019), Vol. 135, pp. 3:1–3:24.
  16. D. J. Rosenbaum, Optimal quantum circuits for nearest-neighbor architectures, in 8th Conference on the Theory of Quantum Computation, Communication and Cryptography (TQC 2013) ( Dagstuhl, Germany, 2013), Vol. 22, pp. 294–307.
  17. P. Pham and K. M. Svore, A 2D nearest-neighbor quantum architecture for factoring in polylogarithmic Depth, Quantum Inf. Comput. 13, 937 (2013).
  18. F. Arute, K. Arya, R. Babbush, D. Bacon, J. C. Bardin, R. Barends, R. Biswas, S. Boixo, F. G. S. L. Brandao, D. A. Buell et al., Quantum supremacy using a programmable superconducting processor, Nature (London) 574, 505 (2019).
  19. M. Saffman, T. G. Walker, and K. Mølmer, Quantum information with Rydberg atoms, Rev. Mod. Phys. 82, 2313 (2010).
  20. H. Weimer, N. Y. Yao, C. R. Laumann, and M. D. Lukin, Long-Range Quantum Gates using Dipolar Crystals, Phys. Rev. Lett. 108, 100501 (2012).
  21. B. Yan, S. A. Moses, B. Gadway, J. P. Covey, K. R. A. Hazzard, A. M. Rey, D. S. Jin, and J. Ye, Observation of dipolar spin-exchange interactions with lattice-confined polar molecules, Nature (London) 501, 521 (2013).
  22. N. Y. Yao, L. Jiang, A. V. Gorshkov, P. C. Maurer, G. Giedke, J. I. Cirac, and M. D. Lukin, Scalable architecture for a room temperature solid-state quantum information processor, Nat. Commun. 3, 800 (2012).
  23. L. Isenhower, M. Saffman, and K. Mølmer, Multibit C k NOT quantum gates via Rydberg blockade, Quant. Info. Proc. 10, 755 (2011).
  24. K. Mølmer, L. Isenhower, and M. Saffman, Efficient Grover search with Rydberg blockade, J. Phys. B: At. Mol. Opt. Phys. 44, 184016 (2011).
  25. D. Petrosyan, Dipolar exchange induced transparency with Rydberg atoms, New J. Phys. 19, 033001 (2017).
  26. J. Gulliksen, D. B. R. Dasari, and K. Mølmer, Characterization of how dissipation and dephasing errors accumulate in quantum computers, EPJ Quantum Technol. 2, 4 (2015).
  27. M. Müller, I. Lesanovsky, H. Weimer, H. P. Büchler, and P. Zoller, Mesoscopic Rydberg Gate Based on Electromagnetically Induced Transparency, Phys. Rev. Lett. 102, 170502 (2009).
  28. J. T. Young, P. Bienias, R. Belyansky, A. M. Kaufman, and A. V. Gorshkov, Asymmetric Blockade and Multi-Qubit Gates Via Dipole-Dipole Interactions, Phys. Rev. Lett. 127, 120501 (2021).
  29. H. Levine, A. Keesling, G. Semeghini, A. Omran, T. T. Wang, S. Ebadi, H. Bernien, M. Greiner, V. Vuletić, H. Pichler, and M. D. Lukin, Parallel Implementation of High-Fidelity Multiqubit Gates with Neutral Atoms, Phys. Rev. Lett. 123, 170503 (2019).
  30. Z. Eldredge, Z.-X. Gong, J. T. Young, A. H. Moosavian, M. Foss-Feig, and A. V. Gorshkov, Fast Quantum State Transfer and Entanglement Renormalization Using Long-Range Interactions, Phys. Rev. Lett. 119, 170503 (2017).
  31. A. Y. Guo, M. C. Tran, A. M. Childs, A. V. Gorshkov, and Z.-X. Gong, Signaling and Scrambling with Strongly Long-Range Interactions, Phys. Rev. A 102, 010401(R) (2020).
  32. M. C. Tran, C.-F. Chen, A. Ehrenberg, A. Y. Guo, A. Deshpande, Y. Hong, Z.-X. Gong, A. V. Gorshkov, and A. Lucas, Hierarchy of Linear Light Cones with Long-Range Interactions, Phys. Rev. X 10, 031009 (2020).
  33. T. Kuwahara and K. Saito, Strictly Linear Light Cones in Long-Range Interacting Systems of Arbitrary Dimensions, Phys. Rev. X 10, 031010 (2020).
  34. We note that in Refs. [54, 55], it was shown that the unbounded quantum fanout could be implemented in trapped-ion systems using a global Molmer-Sorensen gate. However, those methods lead to gate durations that scale superlinearly in the system size in order to achieve a certain value of state fidelity and, as such, do not yield an asymptotic speed-up.
  35. M. C. Tran, A. Y. Guo, A. Deshpande, A. Lucas, and A. V. Gorshkov, Optimal State Transfer and Entanglement Generation in Power-Law Interacting Systems, Phys. Rev. X 11, 031016 (2021).
  36. D. Coppersmith, IBM Technical Report No. RC19642 (1994), arXiv:quant-ph/0201067.
  37. A. V. Gorshkov, A. M. Rey, A. J. Daley, M. M. Boyd, J. Ye, P. Zoller, and M. D. Lukin, Alkaline-Earth-Metal Atoms as Few-Qubit Quantum Registers, Phys. Rev. Lett. 102, 110503 (2009).
  38. See Supplemental Material at http://link.aps.org/supplemental/10.1103/PhysRevResearch.4.L042016 for more details on the implementation of the fanout protocol in a dipolar system as well as a detailed proof of the Theorem.
  39. R. Cleve and J. Watrous, Fast parallel circuits for the quantum Fourier transform, in Proceedings of the 41st Annual Symposium on Foundations of Computer Science, FOCS '00 (IEEE Computer Society, New York, 2000), p. 526.
  40. H. W. Lenstra and C. Pomerance, A rigorous time bound for factoring integers, J. Amer. Math. Soc. 5, 483 (1992).
  41. T. J. Osborne, Efficient Approximation of the Dynamics of One-Dimensional Quantum Spin Systems, Phys. Rev. Lett. 97, 157202 (2006).
  42. We note that a similar result could have been achieved using the fact that constant-depth quantum circuits with two fanouts are not strongly classically simulable unless P=PP [56].
  43. D. Maslov, Linear depth stabilizer and quantum Fourier transformation circuits with no auxiliary qubits in finite neighbor quantum architectures, Phys. Rev. A 76, 052310 (2007).
  44. E. H. Lieb and D. W. Robinson, The finite group velocity of quantum spin systems, Commun. Math. Phys. 28, 251 (1972).
  45. C.-F. Chen and A. Lucas, Finite Speed of Quantum Scrambling with Long Range Interactions, Phys. Rev. Lett. 123, 250605 (2019).
  46. See Ref.  [32] for a more precise definition. We note that our projector Qr is a variation on the Qr used in Ref.  [32]. Specifically, for D=1, they are related via Qr=∑x:|x|≥rQx.
  47. M. C. Tran, A. Y. Guo, Y. Su, J. R. Garrison, Z. Eldredge, M. Foss-Feig, A. M. Childs, and A. V. Gorshkov, Locality and Digital Quantum Simulation of Power-Law Interactions, Phys. Rev. X 9, 031006 (2019).
  48. M. B. Hastings and T. Koma, Spectral gap and exponential decay of correlations, Commun. Math. Phys. 265, 781 (2006).
  49. M. C. Tran, A. Y. Guo, C. L. Baldwin, A. Ehrenberg, A. V. Gorshkov, and A. Lucas, Lieb-Robinson Light Cone for Power-Law Interactions, Phys. Rev. Lett. 127, 160401 (2021).
  50. T. Kuwahara and K. Saito, Absence of Fast Scrambling in Thermodynamically Stable Long-Range Interacting Systems, Phys. Rev. Lett. 126, 030604 (2021).
  51. C.-F. Chen and A. Lucas, Optimal frobenius light cone in spin chains with power-law interactions, Phys. Rev. A 104, 062420 (2021).
  52. J. M. Epstein and K. B. Whaley, Quantum speed limits for quantum-information-processing tasks, Phys. Rev. A 95, 042314 (2017).
  53. Specifically, for even n, this mapping is defined by qi↦q2i−1 for i≤n/2 and qi↦q2(n−i+1) for i>n/2.
  54. D. Maslov and Y. Nam, Use of global interactions in efficient quantum circuit constructions, New J. Phys. 20, 033018 (2018).
  55. Y. Lu, S. Zhang, K. Zhang, W. Chen, Y. Shen, J. Zhang, J.-N. Zhang, and K. Kim, Global entangling gates on arbitrary ion qubits, Nature (London) 572, 363 (2019).
  56. Y. Takahashi, T. Yamazaki, and K. Tanaka, Hardness of classically simulating quantum circuits with unbounded Toffoli and fan-out gates, Quantum Inf. Comput. 14, 1149 (2014).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation