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arxiv: 2107.09676 · v1 · pith:DUQ3BZOP · submitted 2021-07-20 · quant-ph · cond-mat.dis-nn· cond-mat.quant-gas· cond-mat.stat-mech· cond-mat.str-el

Realizing a dynamical topological phase in a trapped-ion quantum simulator

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classification quant-ph cond-mat.dis-nncond-mat.quant-gascond-mat.stat-mechcond-mat.str-el
keywords quantumdynamicaledgeerrorsphasetopologicalworkcontrol
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Nascent platforms for programmable quantum simulation offer unprecedented access to new regimes of far-from-equilibrium quantum many-body dynamics in (approximately) isolated systems. Here, achieving precise control over quantum many-body entanglement is an essential task for quantum sensing and computation. Extensive theoretical work suggests that these capabilities can enable dynamical phases and critical phenomena that exhibit topologically-robust methods to create, protect, and manipulate quantum entanglement that self-correct against large classes of errors. However, to date, experimental realizations have been confined to classical (non-entangled) symmetry-breaking orders. In this work, we demonstrate an emergent dynamical symmetry protected topological phase (EDSPT), in a quasiperiodically-driven array of ten $^{171}\text{Yb}^+$ hyperfine qubits in Honeywell's System Model H1 trapped-ion quantum processor. This phase exhibits 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 orders that would enable error-resilient techniques to manipulate quantum information.

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Cited by 1 Pith paper

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  1. Efimov Effect in Long-range Quantum Spin Chains

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    Long-range interactions in quantum spin chains enable the Efimov effect for magnons by inducing continuous scale invariance in two-body states that becomes discrete in the three-body problem.