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Related Concept Videos

Superconductor01:24

Superconductor

A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
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A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
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Superconducting qubit with Purcell protection and tunable coupling.

J M Gambetta1, A A Houck, Alexandre Blais

  • 1Department of Applied Mathematics, Institute for Quantum Computing, University of Waterloo, Waterloo, Ontario, Canada N2L 3G1.

Physical Review Letters
|March 17, 2011
PubMed
Summary

We developed a tunable superconducting qubit for circuit quantum electrodynamics. This qubit can be tuned to a decoherence-free subspace, suppressing Purcell effect-induced spontaneous emission while enabling qubit measurement.

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Area of Science:

  • Quantum computing
  • Superconducting circuits
  • Quantum information science

Background:

  • Circuit Quantum Electrodynamics (cQED) architecture is a leading platform for superconducting qubits.
  • The Purcell effect, caused by spontaneous emission, is a major source of decoherence in cQED systems.
  • Controlling qubit-resonator coupling is crucial for both qubit operation and mitigating decoherence.

Purpose of the Study:

  • To introduce a superconducting qubit with tunable coupling to its resonator.
  • To demonstrate the creation of a decoherence-free subspace by tuning the coupling strength to zero.
  • To show that qubit measurement is still possible within this decoherence-free subspace.

Main Methods:

  • Implementation of a superconducting qubit within the cQED architecture.
  • Precise tuning of the qubit-resonator coupling strength, denoted as 'g'.
  • Characterization of qubit dynamics and measurement protocols at varying coupling strengths, particularly at g = 0.

Main Results:

  • The qubit-resonator coupling strength 'g' is tunable from zero to values comparable to other superconducting qubits.
  • At g = 0, the qubit resides in a decoherence-free subspace, effectively suppressing spontaneous emission due to the Purcell effect.
  • Qubit state readout is demonstrated within the decoherence-free subspace using dispersive shifts on the resonator's frequency and cycling-type measurements.

Conclusions:

  • A tunable superconducting qubit architecture is presented that allows access to a decoherence-free subspace.
  • This approach mitigates Purcell-limited decay while preserving the ability to measure the qubit state.
  • The tunable coupling offers a new pathway for improving coherence times and control in superconducting quantum processors.