Niobium coaxial cavities with internal quality factors exceeding 1.5 billion for circuit quantum electrodynamics

  1. Andrew E. Oriani,
  2. Fang Zhao,
  3. Tanay Roy,
  4. Alexander Anferov,
  5. Kevin He,
  6. Ankur Agrawal,
  7. Riju Banerjee,
  8. Srivatsan Chakram,
  9. and David I. Schuster
Group-V materials such as niobium and tantalum have become popular choices for extending the performance of circuit quantum electrodynamics (cQED) platforms allowing for quantum processors
and memories with reduced error rates and more modes. The complex surface chemistry of niobium however makes identifying the main modes of decoherence difficult at millikelvin temperatures and single-photon powers. We use niobium coaxial quarter-wave cavities to study the impact of etch chemistry, prolonged atmospheric exposure, and the significance of cavity conditions prior to and during cooldown, in particular niobium hydride evolution, on single-photon coherence. We demonstrate cavities with quality factors of Qint≳1.4×109 in the single-photon regime, a 15 fold improvement over aluminum cavities of the same geometry. We rigorously quantify the sensitivity of our fabrication process to various loss mechanisms and demonstrate a 2−4× reduction in the two-level system (TLS) loss tangent and a 3−5× improvement in the residual resistivity over traditional BCP etching techniques. Finally, we demonstrate transmon integration and coherent cavity control while maintaining a cavity coherence of \SI{11.3}{ms}. The accessibility of our method, which can easily be replicated in academic-lab settings, and the demonstration of its performance mark an advancement in 3D cQED.

The QICK (Quantum Instrumentation Control Kit): Readout and control for qubits and detectors

  1. Leandro Stefanazzi,
  2. Ken Treptow,
  3. Neal Wilcer,
  4. Chris Stoughton,
  5. Salvatore Montella,
  6. Collin Bradford,
  7. Gustavo Cancelo,
  8. Shefali Saxena,
  9. Horacio Arnaldi,
  10. Sara Sussman,
  11. Andrew Houck,
  12. Ankur Agrawal,
  13. Helin Zhang,
  14. Chunyang Ding,
  15. and David I. Schuster
We introduce a Xilinx RFSoC-based qubit controller (called the Quantum Instrumentation Control Kit, or QICK for short) which supports the direct synthesis of control pulses with carrier
frequencies of up to 6 GHz. The QICK can control multiple qubits or other quantum devices. The QICK consists of a digital board hosting an RFSoC (RF System-on-Chip) FPGA \cite{zcu111}, custom firmware and software and an optional companion custom-designed analog front-end board. We characterize the analog performance of the system, as well as its digital latency, important for quantum error correction and feedback protocols. We benchmark the controller by performing standard characterizations of a transmon qubit. We achieve an average Clifford gate fidelity of avg=99.93%. All of the schematics, firmware, and software are open-source \cite{QICKrepo}.

Seamless high-Q microwave cavities for multimode circuit QED

  1. Srivatsan Chakram,
  2. Andrew E. Oriani,
  3. Ravi K. Naik,
  4. Akash V. Dixit,
  5. Kevin He,
  6. Ankur Agrawal,
  7. Hyeokshin Kwon,
  8. and David I. Schuster
Multimode cavity quantum electrodynamics —where a two level system interacts simultaneously with many cavity modes—provides a versatile framework for quantum information
processing and quantum optics. Due to the combination of long coherence times and large interaction strengths, one of the leading experimental platforms for cavity QED involves coupling a superconducting circuit to a 3D microwave cavity. In this work, we realize a 3D multimode circuit QED system with single photon lifetimes of 2 ms and cooperativities of 0.5−1.5×109 across 9 modes of a novel seamless cavity. We demonstrate a variety of protocols for universal single-mode quantum control applicable across all cavity modes, using only a single drive line. We achieve this by developing a straightforward flute method for creating monolithic superconducting microwave cavities that reduces loss while simultaneously allowing control of the mode spectrum and mode-qubit interaction. We highlight the flexibility and ease of implementation of this technique by using it to fabricate a variety of 3D cavity geometries, providing a template for engineering multimode quantum systems with exceptionally low dissipation. This work is an important step towards realizing hardware efficient random access quantum memories and processors, and for exploring quantum many-body physics with photons.

Searching for Dark Matter with a Superconducting Qubit

  1. Akash V. Dixit,
  2. Srivatsan Chakram,
  3. Kevin He,
  4. Ankur Agrawal,
  5. Ravi K. Naik,
  6. David I. Schuster,
  7. and Aaron Chou
The gravitational evidence for the existence of dark matter is extensive, yet thus far, dark matter has evaded direct detection in terrestrial experiments. Detection mechanisms for
low mass dark matter candidates such as the axion or hidden photon leverage potential interactions with electromagnetic fields, whereby the dark matter (of unknown mass) on rare occasion converts into a single photon. Current dark matter searches operating at microwave frequencies, use a resonant cavity to coherently accumulate the field sourced by the dark matter and use a quantum limited linear amplifier to read out the cavity signal. Here, we report the development of a novel microwave photon counting technique and use it to set a new exclusion limit on hidden photon dark matter. We constrain the kinetic mixing angle to ϵ≤1.82×10−15 in a narrow band around 6.011 GHz (24.86 μeV) with an integration time of 8.33 s. We operate a superconducting qubit to make repeated quantum non-demolition measurements of cavity photons and apply a hidden Markov model analysis to reduce the noise to 15.7 dB below the quantum limit, with performance limited by the residual population of the system. The techniques presented here will dramatically improve the sensitivity of future dark matter searches in the range of 3-30 GHz and are generally applicable to measurements that require high sensitivity to inherently low signal photon rates.