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相关概念视频

NMR Spectrometers: Resolution and Error Correction01:14

NMR Spectrometers: Resolution and Error Correction

765
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...
765
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

999
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.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
999
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.0K
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,...
1.0K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.1K
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...
1.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)

1.1K
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.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.1K
Quantum Numbers02:43

Quantum Numbers

35.5K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
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相关实验视频

Updated: Aug 31, 2025

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
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Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

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使用自旋量子比特进行量子错误校正

Kenta Takeda1, Akito Noiri2, Takashi Nakajima2

  • 1Center for Emergent Matter Science (CEMS), RIKEN, Wako, Japan. kenta.takeda@riken.jp.

Nature
|August 24, 2022
PubMed
概括
此摘要是机器生成的。

研究人员使用三量子位系统在中演示量子误差校正 (QEC). 这一突破保护了量子信息,

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Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
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相关实验视频

Last Updated: Aug 31, 2025

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Measurement of Quantum Interference in a Silicon Ring Resonator Photon Source
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科学领域:

  • 量子计算
  • 量子错误纠正
  • 固态物理

背景情况:

  • 大型量子计算机需要量子错误校正 (QEC) 来保护量子信息.
  • 基于的自旋量子比特由于成熟的纳米制造而有望扩展量子设备.
  • 需要多个合量子位的QEC仍然是一个重大挑战.

研究的目的:

  • 在中展示一个三量子位相位校正代码.
  • 展示编码的量子状态对相变错误的保护.
  • 验证量子比特在可扩展量子计算中的潜力.

主要方法:

  • 一个三量子比特的阶段校正代码的演示.
  • 使用iToffoli门实现三量子比特条件旋转.
  • 防止单量子位相变错误和脱相.

主要成果:

  • 在中成功实现三量子位相位校正代码.
  • 减轻单量子位相位翻转和脱相的错误.
  • 一个高效的单步iToffoli门的演示,用于纠错.

结论:

  • 这项研究成功地在基于的平台上证明了量子错误校正.
  • 这些结果突显了自旋量子比特在构建可扩展量子计算机方面的潜力.
  • 这项工作解决了实现容错量子计算的关键挑战.