Microwave-Activated Controlled-Z Gate for Fixed-Frequency Fluxonium Qubits

  1. Konstantin N. Nesterov,
  2. Ivan V. Pechenezhskiy,
  3. Chen Wang,
  4. Vladimir E. Manucharyan,
  5. and Maxim G. Vavilov
The superconducting fluxonium circuit is an artificial atom with a strongly anharmonic spectrum: when biased at a half flux quantum, the lowest qubit transition is an order of magnitude
smaller in frequency than those to higher levels. Similar to conventional atomic systems, such a frequency separation between the computational and noncomputational subspaces allows independent optimizations of the qubit coherence and two-qubit interactions. Here we describe a controlled-Z gate for two fluxoniums connected either capacitively or inductively, with qubit transitions fixed near 500 MHz. The gate is activated by a microwave drive at a resonance involving the second excited state. We estimate intrinsic gate fidelities over 99.9% with gate times below 100 ns.

Controlled-Z gate for transmon qubits coupled by semiconductor junctions

  1. Zhenyi Qi,
  2. Hong-Yi Xie,
  3. Javad Shabani,
  4. Vladimir E. Manucharyan,
  5. Alex Levchenko,
  6. and Maxim G. Vavilov
We analyze the coupling of two qubits via an epitaxial semiconducting junction. In particular, we consider three configurations that include pairs of transmons or gatemons as well as
gatemon-like two qubits formed by an epitaxial four-terminal junction. These three configurations provide an electrical control of the interaction between the qubits by applying voltage to a metallic gate near the semiconductor junction and can be utilized to naturally realize a controlled-Z gate (CZ). We calculate the fidelity and timing for such CZ gate. We demonstrate that in the absence of decoherence, the CZ gate can be performed under 50 ns with gate error below 10−4.

Scalable two- and four-qubit parity measurement with a threshold photon counter

  1. Luke C.G. Govia,
  2. Emily J. Pritchett,
  3. B. L. T. Plourde,
  4. Maxim G. Vavilov,
  5. R. McDermott,
  6. and Frank K. Wilhelm
Parity measurement is a central tool to many quantum information processing tasks. In this Letter, we propose a method to directly measure two- and four-qubit parity with low overhead
in hard- and software, while remaining robust to experimental imperfections. Our scheme relies on dispersive qubit-cavity coupling and photon counting that is sensitive only to intensity; both ingredients are widely realized in many different quantum computing modalities. For a leading technology in quantum computing, superconducting integrated circuits, we analyze the measurement contrast and the back action of the scheme and show that this measurement comes close enough to an ideal parity measurement to be applicable to quantum error correction.

High-fidelity qubit measurement with a microwave photon counter

  1. Luke C.G. Govia,
  2. Emily J. Pritchett,
  3. Canran Xu,
  4. B. L. T. Plourde,
  5. Maxim G. Vavilov,
  6. Frank K. Wilhelm,
  7. and R. McDermott
High-fidelity, efficient quantum nondemolition readout of quantum bits is integral to the goal of quantum computation. As superconducting circuits approach the requirements of scalable,
universal fault tolerance, qubit readout must also meet the demand of simplicity to scale with growing system size. Here we propose a fast, high-fidelity, scalable measurement scheme based on the state-selective ring-up of a cavity followed by photodetection with the recently introduced Josephson photomultiplier (JPM), a current-biased Josephson junction. This scheme maps qubit state information to the binary digital output of the JPM, circumventing the need for room-temperature heterodyne detection and offering the possibility of a cryogenic interface to superconducting digital control circuitry. Numerics show that measurement contrast in excess of 95% is achievable in a measurement time of 140 ns. We discuss perspectives to scale this scheme to enable readout of multiple qubit channels with a single JPM.