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NMR Spectrometers: Resolution and Error Correction01:14

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When magnetic nuclei in a sample achieve resonance and undergo relaxation, the signal detected in NMR is an approximately exponential free induction decay. Fourier transform of an exponential decay yields a Lorentzian peak in the frequency domain. Lorentzian peaks in an NMR spectrum are defined by their amplitude, full width at half maximum, and position, where the peak width is governed by the spin-spin relaxation time alone. In real experiments, however, the applied magnetic field is rendered...
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To achieve precise distance measurements, especially in surveying and construction, certain corrections must be applied to account for potential sources of error like the standardization errors, temperature variations, and slope adjustments.Standardization error emerges when measurement equipment undergoes changes, such as wear, repairs, or weather impacts. To address this, surveyors compare the equipment’s readings to a standard. This process identifies any deviation that might lead to...
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The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this...
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Quantum Numbers02:43

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Related Experiment Video

Updated: Aug 24, 2025

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
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Single-shot quantum error correction with the three-dimensional subsystem toric code.

Aleksander Kubica1,2,3,4, Michael Vasmer5,6

  • 1Perimeter Institute for Theoretical Physics, Waterloo, ON, N2L 2Y5, Canada. akubica@caltech.edu.

Nature Communications
|October 21, 2022
PubMed
Summary
This summary is machine-generated.

Researchers developed a new 3D subsystem toric code for quantum error correction (QEC). This code offers efficient, single-shot QEC with a high threshold, making fault-tolerant quantum computing more achievable.

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Area of Science:

  • Quantum Computing
  • Quantum Error Correction

Background:

  • Quantum computers require fault-tolerant protocols and quantum error correction (QEC) to overcome inherent component errors.
  • Optimizing resource and time overheads for QEC is a critical challenge in quantum computing development.

Purpose of the Study:

  • Introduce a novel topological quantum error-correcting code: the three-dimensional subsystem toric code (3D STC).
  • Demonstrate the efficiency and reliability of the 3D STC for practical quantum error correction.

Main Methods:

  • The 3D STC is implemented using geometrically-local parity checks with a maximum weight of three on a cubic lattice with open boundary conditions.
  • Proved that a single round of parity-check measurements is sufficient for reliable QEC, even with measurement errors.
  • Developed an efficient single-shot QEC decoding strategy tailored for the 3D STC.

Main Results:

  • The 3D STC enables reliable quantum error correction with geometrically-local parity checks.
  • A single round of parity-check measurements is sufficient for effective QEC, even with measurement errors.
  • Numerical estimation shows a storage threshold of approximately 1.045% against independent bit-flip, phase-flip, and measurement errors.

Conclusions:

  • The 3D STC offers a promising approach for fault-tolerant quantum computing due to its high threshold and local parity-check requirements.
  • The code's efficiency and reliability make it a strong candidate for practical implementation in future quantum computers.