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相关概念视频

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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Atomic Nuclei: Nuclear Spin01:08

Atomic Nuclei: Nuclear Spin

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All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not...
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Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

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Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
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Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

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In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis,  the precessing magnetic moments are randomly oriented around the z-axis.
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Atomic Nuclei: Magnetic Resonance01:05

Atomic Nuclei: Magnetic Resonance

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The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
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The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

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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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Gradient Echo Quantum Memory in Warm Atomic Vapor
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固态量子比特的核旋波量子寄存器

Andrei Ruskuc1,2,3, Chun-Ju Wu1,2,3,4, Jake Rochman1,2,3

  • 1Thomas J. Watson, Sr., Laboratory of Applied Physics, California Institute of Technology, Pasadena, CA, USA.

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概括
此摘要是机器生成的。

研究人员使用伊金的核旋转开发了一种量子记忆. 这一突破利用集体自旋激发来进行强大的量子信息存储和纠, 进步量子网络.

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科学领域:

  • 量子信息科学
  • 固态量子系统
  • 量子计算和网络

背景情况:

  • 对于量子技术来说,光学地址化的固态核旋转至关重要.
  • 核丰富的宿主虽然由于脱而具有挑战性, 但却提供了独特的量子存储潜力.
  • 之前的努力并没有利用密集的核旋转组合来控制单旋转量子位.

研究的目的:

  • 开发一个量子控制协议来操纵密集环境中的核自旋状态.
  • 用集体核自旋激发来实现量子内存.
  • 探索用于强大的量子信息应用的富含核旋转的主机.

主要方法:

  • 使用了高连贯性,光学地址的伊特-171 (Yb3+) 量子位.
  • 开发了一种动态的旋转交换相互作用,以极化和激发邻近的-51 (V5+) 核旋转组合.
  • 实现了量子记忆,并展示了纠的贝尔状态的准备和测量.

主要成果:

  • 成功地使密集的核旋转组合两极化,并产生集体旋转激发.
  • 基于这些集体激发实现了确定性和可重现的量子记忆.
  • 演示了最大纠的171-51V钟状态的创建和测量.

结论:

  • 开发的量子控制协议允许使用密集的核自旋浴作为量子资源.
  • 这种平台提供了一种决定性和可重现的量子记忆方法, 与传统的无序系统不同.
  • 这些发现为在核丰富材料中使用单个稀土离子量子比特构建大规模量子网络铺平了道路.