Observation of topological transitions in interacting quantum circuits

Topology, with its abstract mathematical constructs, often manifests itself in physics and has a pivotal role in our understanding of natural phenomena. Notably, the discovery of topological phases in condensed-matter systems has changed the modern conception of phases of matter. The global nature of topological ordering, however, makes direct experimental probing an outstanding challenge. Present experimental tools are mainly indirect and, as a result, are inadequate for studying the topology of physical systems at a fundamental level. Here we employ the exquisite control afforded by state-of-the-art superconducting quantum circuits to investigate topological properties of various quantum systems. The essence of our approach is to infer geometric curvature by measuring the deflection of quantum trajectories in the curved space of the Hamiltonian. Topological properties are then revealed by integrating the curvature over closed surfaces, a quantum analogue of the Gauss–Bonnet theorem. We benchmark our technique by investigating basic topological concepts of the historically important Haldane model after mapping the momentum space of this condensed-matter model to the parameter space of a single-qubit Hamiltonian. In addition to constructing the topological phase diagram, we are able to visualize the microscopic spin texture of the associated states and their evolution across a topological phase transition. Going beyond non-interacting systems, we demonstrate the power of our method by studying topology in an interacting quantum system. This required a new qubit architecture that allows for simultaneous control over every term in a two-qubit Hamiltonian. By exploring the parameter space of this Hamiltonian, we discover the emergence of an interaction-induced topological phase. Our work establishes a powerful, generalizable experimental platform to study topological phenomena in quantum systems.

[1]  K. Cheng Theory of Superconductivity , 1948, Nature.

[2]  R. Barends,et al.  Coherent Josephson qubit suitable for scalable quantum integrated circuits. , 2013, Physical review letters.

[3]  Haldane,et al.  Model for a quantum Hall effect without Landau levels: Condensed-matter realization of the "parity anomaly" , 1988, Physical review letters.

[4]  Erik Lucero,et al.  Implementing the Quantum von Neumann Architecture with Superconducting Circuits , 2011, Science.

[5]  B. Bernevig Topological Insulators and Topological Superconductors , 2013 .

[6]  F. Wilczek,et al.  Geometric Phases in Physics , 1989 .

[7]  C. Kane,et al.  Topological Insulators , 2019, Electromagnetic Anisotropy and Bianisotropy.

[8]  M. Berry Quantal phase factors accompanying adiabatic changes , 1984, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[9]  A N Cleland,et al.  Qubit Architecture with High Coherence and Fast Tunable Coupling. , 2014, Physical review letters.

[10]  A. Polkovnikov,et al.  Dynamical quantum Hall effect in the parameter space , 2011, Proceedings of the National Academy of Sciences.

[11]  J. García-Ripoll,et al.  Detection of Chern numbers and entanglement in topological two-species systems through subsystem winding numbers , 2014, 1402.3222.

[12]  P. Dirac Quantised Singularities in the Electromagnetic Field , 1931 .

[13]  R. J. Schoelkopf,et al.  Observation of Berry's Phase in a Solid-State Qubit , 2007, Science.

[14]  J. Neumann,et al.  Über merkwürdige diskrete Eigenwerte , 1993 .

[15]  Shou-Cheng Zhang,et al.  Quantum Spin Hall Effect and Topological Phase Transition in HgTe Quantum Wells , 2006, Science.

[16]  Anatoli Polkovnikov,et al.  Measuring a topological transition in an artificial spin-1/2 system. , 2014, Physical review letters.

[17]  Yize Jin,et al.  Topological insulators , 2014, Topology in Condensed Matter.

[18]  F. Nori,et al.  Quantum Simulators , 2009, Science.

[19]  G. Dorda,et al.  New Method for High-Accuracy Determination of the Fine-Structure Constant Based on Quantized Hall Resistance , 1980 .

[20]  Nonadiabatic dynamics of a slowly driven dissipative two-level system , 2014, 1402.4210.

[21]  Joel E Moore,et al.  The birth of topological insulators , 2010, Nature.

[22]  Charles Neill,et al.  Tunable coupler for superconducting Xmon qubits: Perturbative nonlinear model , 2014, 1405.1915.

[23]  Immanuel Bloch,et al.  Direct measurement of the Zak phase in topological Bloch bands , 2012, Nature Physics.

[24]  John M. Martinis,et al.  Logic gates at the surface code threshold: Superconducting qubits poised for fault-tolerant quantum computing , 2014 .

[25]  Erik Lucero,et al.  Emulation of a Quantum Spin with a Superconducting Phase Qudit , 2009, Science.

[26]  Marco Lanzagorta,et al.  Quantum Simulators , 2013 .

[27]  W. Marsden I and J , 2012 .

[28]  D. C. Tsui,et al.  Two-Dimensional Magnetotransport in the Extreme Quantum Limit , 1982 .

[29]  D. Thouless,et al.  Quantized Hall conductance in a two-dimensional periodic potential , 1992 .

[30]  R. Feynman Simulating physics with computers , 1999 .

[31]  A. Houck,et al.  On-chip quantum simulation with superconducting circuits , 2012, Nature Physics.