Quasiperiodic circuit quantum electrodynamics

  1. Tobias Herrig,
  2. Jedediah H. Pixley,
  3. Elio J. König,
  4. and Roman-Pascal Riwar
Superconducting circuits are an extremely versatile platform to realize quantum information hardware, and, as was recently realized, to emulate topological materials, such as three-dimensional
Weyl semimetals or two-dimensional Chern insulators. We here show how a simple arrangement of capacitors and conventional superconductor-insulator-superconductor (SIS) junctions can realize a nonlinear capacitive element with a surprising property: it can be quasiperiodic with respect to the quantized Cooper-pair charge. Integrating this element into a larger circuit opens the door towards the engineering of an even broader class of systems. First, we use it to simulate a protected Dirac material defined in the transport degrees of freedom. The presence of the Dirac points leads to a suppression of the classical part of the finite-frequency current noise. Second, we exploit the quasiperiodicity to implement the Aubry-André model, and thereby emulate Anderson localization in charge space. Importantly, the realization by means of transport degrees of freedom allows for a straightforward generalization to arbitrary dimensions. Moreover, our setup implements a truly non-interacting version of the model, in which the macroscopic quantum mechanics of the circuit already incorporates microscopic interaction effects. We propose that measurements of the quantum fluctuations of the charge can be used to directly probe the localization effect. Finally, we present an outlook in which the nonlinear capacitance is employed in a quantum circuit emulating a magic-angle effect akin to twisted bilayer graphene.

A „minimal“ topological quantum circuit

  1. Tobias Herrig,
  2. and Roman-Pascal Riwar
The outlook of protected quantum computing spurred enormous progress in the search for topological materials, sustaining a continued race to find the most experimentally feasible platform.
Here, we show that one of the simplest quantum circuits, the Cooper-pair transistor, exhibits a nontrivial Chern number which has not yet been discussed, in spite of the exhaustive existing literature. Surprisingly, the resulting quantized current response is robust with respect to a large number of external perturbations, most notably low-frequency charge noise and quasiparticle poisoning. Moreover, the fact that the higher bands experience crossings with higher topological charge leads to all the bands having the same Chern number, such that there is no restriction to stay close to the ground state. Remaining small perturbations are investigated based on a generic Master equation approach. Finally, we discuss feasible protocols to measure the quantized current.