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相关概念视频

¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

1.0K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
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The de Broglie Wavelength02:32

The de Broglie Wavelength

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In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
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NMR Spectroscopy: Spin–Spin Coupling01:08

NMR Spectroscopy: Spin–Spin Coupling

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The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.3K
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)01:20

¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)

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When proton-coupled carbon-13 spectra are simplified by a broadband proton decoupling technique, structural information about the coupled protons is lost. Distortionless enhancement by polarization transfer (DEPT) is a technique that provides information on the number of hydrogens attached to each carbon in a molecule. While the DEPT experiment utilizes complex pulse sequences, the pulse delay and flip angle are specifically manipulated. The resulting signals have different phases depending on...
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The Quantum-Mechanical Model of an Atom02:45

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
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Hybridization of Atomic Orbitals II03:35

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sp3d and sp3d 2 Hybridization
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在分子4f量子比特中探测脱凝.

Steen H Hansen1, Christian D Buch1, Jonatan B Petersen2

  • 1Department of Chemistry, University of Copenhagen DK-2100 Copenhagen Denmark piligkos@chem.ku.dk.

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概括

分子磁性材料表现出很长的连贯时间,这对于量子技术至关重要. 研究表明,光谱扩散在低电场上限制了连贯性,而在高电场上则占主导地位.

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科学领域:

  • 量子信息科学是一种量子信息科学.
  • 分子磁力学分子磁力学
  • 固态物理 固态物理

背景情况:

  • 不连贯性限制了量子计算.
  • 分子磁性材料为量子应用提供了潜力.
  • 了解脱凝机制是量子比特开发的关键.

研究的目的:

  • 为了研究导致分子磁性材料脱凝的因素.
  • 为了确定X频段频率的相位记忆时间 (Tm).
  • 为了比较不同磁场和兴奋剂水平的脱凝性.

主要方法:

  • 脉冲电子偏磁共振 (EPR) 光谱在X频段 (∼9.6 GHz).
  • 哈恩回声,部分重定焦和CPMG脉冲序列使用.
  • 在各种兴奋剂水平 (0.5%至10−3%) 上测量了Gd@Y(trensal) 单晶.

主要成果:

  • 在X频段的相位记忆时间 (Tm) 在5K时从1-12μs不等.
  • 在高于液 (125 K) 的温度下保持一致性.
  • 在低电场时,光谱扩散限制了Tm;在高电场时,自旋格子放松是限制性的.

结论:

  • Gd@Y(trensal) 在X频段表现出显著的连贯性,适合量子信息处理.
  • 在动态解下实现的高量子比特优点 (99.99%的忠实性).
  • 这些发现为开发在更高温度下运行的分子量子比特铺平了道路.