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Dynamical topological phase realized in a trapped-ion quantum simulator


Nascent platforms for programmable quantum simulation offer unprecedented access to new regimes of far-from-equilibrium quantum many-body dynamics in almost isolated systems. Here achieving precise control over quantum many-body entanglement is an essential task for quantum sensing and computation. Extensive theoretical work indicates that these capabilities can enable dynamical phases and critical phenomena that show topologically robust methods to create, protect and manipulate quantum entanglement that self-correct against large classes of errors. However, so far, experimental realizations have been confined to classical (non-entangled) symmetry-breaking orders1,2,3,4,5. In this work, we demonstrate an emergent dynamical symmetry-protected topological phase6, in a quasiperiodically driven array of ten 171Yb+ hyperfine qubits in Quantinuum’s System Model H1 trapped-ion quantum processor7. This phase shows edge qubits that are dynamically protected from control errors, cross-talk and stray fields. Crucially, this edge protection relies purely on emergent dynamical symmetries that are absolutely stable to generic coherent perturbations. This property is special to quasiperiodically driven systems: as we demonstrate, the analogous edge states of a periodically driven qubit array are vulnerable to symmetry-breaking errors and quickly decohere. Our work paves the way for implementation of more complex dynamical topological orders8,9 that would enable error-resilient manipulation of quantum information.

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Fig. 1: Fibonacci drive (EDSPT).
Fig. 2: Floquet drive (FSPT).

Data availability

The data contained in the figures of the main text and the extended data are available for download at

Code availability

The software used in this manuscript are available from the corresponding authors upon request.


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We thank Y. Zhang and M. Foss-Feig for discussions, as well as D. V. Else, A. J. Friedman, W. W. Ho and B. Ware for previous collaboration on this topic. We thank the entire Quantinuum team for their many contributions. This work was supported by National Science Federation Convergence Accelerator Track C award no. 2040549 (A.C.P.), the US Department of Energy, Office of Science, Basic Energy Sciences, under Early Career award no. DE-SC0019168 (R.V.), and the Alfred P. Sloan Foundation through Sloan Research Fellowships (R.V. and A.C.P.). This research was undertaken thanks, in part, to funding from the Max Planck-UBC-UTokyo Center for Quantum Materials and the Canada First Research Excellence Fund, Quantum Materials and Future Technologies Program (A.C.P.). The Flatiron Institute is a division of the Simons Foundation. Numerical simulations were performed in part on the Lonestar5 supercomputing system at the Texas Advanced Computing Center at the University of Texas, Austin.

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Authors and Affiliations



J.G.B., J.P.G., A.H., D.H. and B.N. all contributed to the experimental design, construction and data collection. P.T.D., A.K., R.V. and A.C.P. contributed to the theory, quantum circuit design and data analysis. All authors contributed to this manuscript.

Corresponding authors

Correspondence to Philipp T. Dumitrescu or Andrew C. Potter.

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The authors declare no competing interests.

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Nature thanks Guido Pagano and the other, anonymous, reviewer(s) for their contribution to the peer review of this work.

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Extended data figures and tables

Extended Data Fig. 1

Circuit compilation. Compilation of two-qubit operations into hardware-native gates for (a) the FSPT model (Fig. 2), and (b) the EDSPT model (Fig. 1). XXθ gates are obtained from a single-qubit basis rotation of ZZθ gates. Here, a line with two dots indicates a controlled-Z gate with unitary: \({u}_{{C}_{Z}}={e}^{-i\pi /4(1+{\sigma }^{z})\otimes (1+{\sigma }^{z})}\), and single qubit gates are listed as Pauli rotations with unitary \({u}_{X,{Y}_{\theta }}={e}^{-i\frac{\theta }{2}{\sigma }^{x,y}}\).

Extended Data Fig. 2 Disorder resolved EDSPT.

Data for edge qubits (top row) and site-averaged bulk qubits (bottom row) for the EDSPT protocol at J = 0.95π (Fig. 1). The different curves correspond to different static disorder realizations of Ki,α and Bα,i. Disorder d0 is performed on the H1-1 quantum device, whilst the other disorders are performed on the newer H1-2 device. See Methods for the differences between these devices. The H1-2 data (disorder averaged) was shown in Fig. 1a. The edge state data for single disorder d0 was shown in Fig. 1b, to compare with other J data taken on the same device.

Extended Data Fig. 3 Global qubit frequency calibration error.

(a) Histogram of the observed difference between the calibrated qubit frequency and the last known good calibration for each of the three ion trap gate zones: G2, G3, and G4. (b) Time-series of same data. These errors arise due to combination of background drifts in the magnetic field environment and statistical error in the actual qubit frequency calibration. For the data detailed in this paper, we observe a global RMS frequency error of ±0.5(1) Hz. Outliers are filtered (dashed line) for points greater than 4x the standard deviation to better capture the average behaviour of this error source.

Extended Data Fig. 4 FSPT Simulation with Coherent Error –.

Classical simulations of the FSPT in the presence of a coherent error of the form Eq. (3) in addition to depolarizing noise. Here, we perform 50 different coherent error realizations, with 104 measurement shots for each. The dark lines indicate the error averaged result for each site i, the pale line is an example of single coherent error realization. The parameters tlayerδf[xi] are drawn from a Gaussian distribution of standard deviation 0.025 and are approximated to be constant in time.

Extended Data Fig. 5 Loschmidt flux echo (ED Simulations).

Exact diagonalization (ED) simulations of the Loschmidt flux echo, \({\mathscr{Z}}(t)\), for the Floquet model with L = 9 for J = 0.9π in the FSPT phase (blue dots) where it exhibits saturating period-two oscillations, J = 0.5 in the thermal phase (purple diamonds) where \({\mathscr{Z}}(t)\) immediately averages to zero, and for J = 0.1π in a trivial MBL phase (orange, triangles) where \({\mathscr{Z}}(t)\) saturates to a non-oscillating value. Each point is averaged over all initial states and 100 disorder realizations.

Extended Data Fig. 6 Loschmidt flux echo.

(a) Interferometric protocol for measuring the Loschmidt flux-echo, \({\mathscr{Z}}(t)\): controlled evolution and measurement of an ancilla a (shown here in red) enables measurement of the overlap between time evolved states with and without a symmetry flux inserted. (b) Circuit for implementing the ancilla-controlled flux insertion. (c) Simulated and experimental data for the Loschmidt flux echo in the Floquet model with J = 0.9π (top panel) in the FSPT phase, J = 0.1π (bottom left panel) in the trivial MBL phase, and J = 0.5π (bottom right panel) in the thermalizing phase. For ideal noiseless simulations (pale line, simulation), symmetry-preserving MBL \({\mathscr{Z}}(t)\) exhibits persistent period-two oscillations in the FSPT phase, saturates to a constant value in the trivial MBL phase, and rapidly decays in the thermalizing phase. For weakly-open but symmetry-preserving MBL systems (dashed line, simulation) the oscillation or saturation amplitude slowly decays due to incoherent errors. By contrast, the experimental data strongly deviates from the symmetric simulations after \(t\gtrsim 5\) Floquet periods due to coherent errors. Experimental data shown for trivial-MBL and thermal include only ten shots, and were taken for a different disorder realization than the FSPT data.

Extended Data Fig. 7 Slow heating (numerical simulations).

Numerical simulations of the long-time behaviour of \(|{C}_{z}|\) for the edge qubit of an L = 10 qubit-chain with the Fibonacci drive, for various J (other parameters chosen as in Fig. 1). Each point is averaged over 960 disorder realizations. The inset shows estimate of heating time th empirically defined as the time when \(|{C}_{z}|\) drops below a small threshold ε = 0.02 (dashed line), and demonstrates that the three-fold periodic oscillations persist to timescale exponentially long in the inverse pulse detuning, \({|J-\pi |}^{-1}\).

Extended Data Fig. 8 Ideal FSPT implementation (short times).

FSPT model simulation (noiseless: pale solid lines, noisy: dashed lines) and experimental data (solid points with error bars) at the ideal J = π “fixed-point”. At these short times t ≤ 15, coherent errors have not yet affected the topological edge qubits. The edge shows the expected period-two oscillations, whereas bulk qubits show slowly decaying, weakly-open MBL behaviour along the symmetry axis σx, and rapidly dephase due to random fields and qubit-qubit interactions perpendicular to the symmetry axis, σz.

Extended Data Fig. 9 EDSPT with uniaxial disorder.

(a) Edge and (site averaged) bulk correlators for various values of J for the EDSPT model with disorder that nominally has a microscopic \({{\mathbb{Z}}}_{2}\) symmetry \(({{\bf{B}}}_{i}\parallel \hat{y})\). This symmetry is broken in the implementation by the same coherent errors that decohere the FSPT edge states. The EDSPT behaviour is not harmed by these coherent errors and does not rely on this fine-tuned symmetry; it persists over a range of \(|\,J-\pi |/\pi \lesssim 0.25\). Pale lines show idealized (noiseless) simulations, dashed lines show simulations with depolarizing noise, and solid dots with 1σ-error bars are experimental data. (b) The same edge data for various J replotted on a single plot to facilitate comparison of curves with different pulse-weights.

Extended Data Fig. 10 EDSPT Site-resolved Correlators (with uniaxial disorder).

shown for each site \(i\in \{1,2,\ldots 10\}\) in the chain. Pale lines show idealized (noiseless) simulations, dashed lines show simulations with depolarizing noise, and solid dots with 1σ-error bars are experimental data. As described in the Methods section, even sites are prepared and measured in the z basis and odd sites in the x basis. Whereas edge sites (i = 1, 10) exhibit period-three oscillations in Fibonacci time, the bulk sites (2 ≤ i ≤ 9) undergo random, but slowly decaying oscillations characteristic of the slow dephasing dynamics of MBL. Upon disorder- and/or site- averaging these random oscillations wash out as presented in Extended Data Fig. 9.

Supplementary information

Supplementary Information

Supplementary methods and calculations that detail the relationship between the dynamic sequences studied to the standard AKLT chain, which present a method to detect FSPT order through many-body interferometry, and which explore the stability of quasiperiodically driven MBL and demonstrate the long time (meta)stability of recursively generated quasiperiodic drives and the theoretical emergence of the multiple time-translation symmetries.

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Dumitrescu, P.T., Bohnet, J.G., Gaebler, J.P. et al. Dynamical topological phase realized in a trapped-ion quantum simulator. Nature 607, 463–467 (2022).

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