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Related Concept Videos

Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

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NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
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Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
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Spin–Spin Coupling: One-Bond Coupling01:17

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Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
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In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
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The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
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Quantum logic with spin qubits crossing the surface code threshold.

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Researchers achieved over 99.5% fidelity for single- and two-qubit gates in a silicon quantum processor. This breakthrough in high-fidelity quantum control paves the way for fault-tolerant quantum computing.

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Area of Science:

  • Quantum Computing
  • Semiconductor Physics

Background:

  • High-fidelity quantum bit (qubit) control is essential for reliable quantum algorithms and fault tolerance.
  • Achieving two-qubit gate fidelities above 99% is a major goal for semiconductor spin qubits, crucial for scalable quantum processors.
  • The surface code, a leading quantum error correction code, requires error rates below approximately 1% for fault tolerance.

Purpose of the Study:

  • To demonstrate a spin-based quantum processor in silicon with exceptionally high single- and two-qubit gate fidelities.
  • To assess the performance of these high-fidelity gates, including crosstalk and idling errors.
  • To execute a complex quantum algorithm, the variational quantum eigensolver, using the developed high-fidelity gate set.

Main Methods:

  • Fabrication and operation of a spin-based quantum processor in silicon.
  • Utilization of gate-set tomography to precisely measure single- and two-qubit gate fidelities.
  • Implementation of the variational quantum eigensolver algorithm for molecular ground-state energy calculations.

Main Results:

  • Achieved single- and two-qubit gate fidelities exceeding 99.5%.
  • Maintained average single-qubit gate fidelities above 99% even when accounting for crosstalk and idling errors.
  • Successfully executed the variational quantum eigensolver algorithm, demonstrating the practical application of the high-fidelity gates.

Conclusions:

  • The developed silicon quantum processor surpasses the critical 99% two-qubit gate fidelity threshold, a key milestone for fault tolerance.
  • Semiconductor spin qubits are now strongly positioned for advancements in fault-tolerant quantum computing.
  • These high-fidelity gates are promising for applications in the current era of noisy intermediate-scale quantum devices.