Widely tunable on-chip microwave circulator for superconducting quantum circuits

  1. Benjamin J. Chapman,
  2. Eric I. Rosenthal,
  3. Joseph Kerckhoff,
  4. Bradley A. Moores,
  5. Leila R. Vale,
  6. Gene C. Hilton,
  7. Kevin Lalumière,
  8. Alexandre Blais,
  9. and K. W. Lehnert
We report on the design and performance of an on-chip microwave circulator with a widely (GHz) tunable operation frequency. Non-reciprocity is created with a combination of frequency
conversion and delay, and requires neither permanent magnets nor microwave control tones, allowing on-chip integration with other superconducting circuits without expensive control hardware. Isolation in the device exceeds 20 dB over a bandwidth of tens of MHz, and its insertion loss is small, reaching as low as 0.9 dB at select operation frequencies. Furthermore, the device is linear with respect to input power for signal powers up to hundreds of fW (≈103 circulating photons), and the direction of circulation can be dynamically reconfigured. We demonstrate its operation at a selection of frequencies between 4 and 6 GHz.

Breaking Lorentz reciprocity with frequency conversion and delay

  1. Eric I. Rosenthal,
  2. Benjamin J. Chapman,
  3. Andrew P. Higginbotham,
  4. Joseph Kerckhoff,
  5. and K. W. Lehnert
We introduce a method for breaking Lorentz reciprocity based upon the non-commutation of frequency conversion and delay. The method requires no magnetic materials or resonant physics,
allowing for the design of scalable and broadband non-reciprocal circuits. With this approach, two types of gyrators — universal building blocks for linear, non-reciprocal circuits — are constructed. Using one of these gyrators, we create a circulator with > 15 dB of isolation across the 5 — 9 GHz band. Our designs may be readily extended to any platform with suitable frequency conversion elements, including semiconducting devices for telecommunication or an on-chip superconducting implementation for quantum information processing.

Single-sideband modulator for frequency domain multiplexing of superconducting qubit readout

  1. Benjamin J. Chapman,
  2. Eric I. Rosenthal,
  3. Joseph Kerckhoff,
  4. Leila R. Vale,
  5. Gene C. Hilton,
  6. and K. W. Lehnert
We introduce and experimentally characterize a superconducting single-sideband modulator compatible with cryogenic microwave circuits, and propose its use for frequency domain multiplexing
of superconducting qubit readout. The monolithic single-quadrature modulators that comprise the device are formed with purely reactive elements (capacitors and Josephson junction inductors) and require no microwave-frequency control tones. Microwave signals in the 4 to 8 GHz band, with power up to -85 dBm, are converted up or down in frequency by as much as 120 MHz. Spurious harmonics in the device can be suppressed by up to 25 dB for select probe and modulation frequencies.

General purpose multiplexing device for cryogenic microwave systems

  1. Benjamin J. Chapman,
  2. Bradley A. Moores,
  3. Eric I. Rosenthal,
  4. Joseph Kerckhoff,
  5. and K. W. Lehnert
We introduce and experimentally characterize a general purpose device for signal processing in circuit quantum electrodynamics systems. The device is a broadband two-port microwave
circuit element with three modes of operation: it can transmit, reflect, or invert incident signals between 4 and 8 GHz. This property makes it a versatile tool for lossless signal processing at cryogenic temperatures. In particular, rapid switching (less than or equal to 15 ns) between these operation modes enables several multiplexing readout protocols for superconducting qubits. We report the device’s performance in a two-channel code domain multiplexing demonstration. The multiplexed data are recovered with fast readout times (up to 400 ns) and infidelities less than 0.01 for probe powers greater than 7 fW, in agreement with the expectation for binary signaling with Gaussian noise.

Closing a quantum feedback loop inside a cryostat: Autonomous state-preparation and long-time memory of a superconducting qubit

  1. Christian Kraglund Andersen,
  2. Joseph Kerckhoff,
  3. Konrad W. Lehnert,
  4. Benjamin J. Chapman,
  5. and Klaus Mølmer
We propose to use a cryogenic nonlinear resonator for the projective readout, classical memory, and feedback for a superconducting qubit. This approach sidesteps many of the inefficiencies
inherent in two-way communication between temperature stages in typical systems with room temperature controllers, and avoids increasing the cryogenic heat load. This controller may find a broad range of uses in multi-qubit systems, but here we analyze two specific demonstrative cases in single qubit-control. In the first case, the nonlinear controller is used to initialize the qubit in a definite eigenstate. And in the second case, the qubit’s state is read into the controller’s classical memory, where it is stored for an indefinite period of time, and then used to reinstate the measured state after the qubit has decayed. We analyze the properties of this system and we show simulations of the time evolution for the full system dynamics.

On-chip superconducting microwave circulator from synthetic rotation

  1. Joseph Kerckhoff,
  2. Kevin Lalumière,
  3. Benjamin J. Chapman,
  4. Alexandre Blais,
  5. and K. W. Lehnert
We analyze the design of a potential replacement technology for the commercial ferrite circulators that are ubiquitous in contemporary quantum superconducting microwave experiments.
The lossless, lumped element design is capable of being integrated on chip with other superconducting microwave devices, thus circumventing the many performance-limiting aspects of ferrite circulators. The design is based on the dynamic modulation of DC superconducting microwave quantum interference devices (SQUIDs) that function as nearly linear, tunable inductors. The connection to familiar ferrite-based circulators is a simple frame boost in the internal dynamics‘ equation of motion. In addition to the general, schematic analysis, we also give an overview of many considerations necessary to achieve a practical design with a tunable center frequency in the 4-8 GHz frequency band, a bandwidth of 240 MHz, reflections at the -20 dB level, and a maximum signal power of approximately order 100 microwave photons per inverse bandwidth.