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

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

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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.
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...
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Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

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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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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.0K
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...
1.0K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

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1.1K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
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Ziegler–Natta Chain-Growth Polymerization: Overview01:17

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Ziegler–Natta polymerization is another form of addition or chain‐growth polymerization used for synthesizing linear polymers over branched polymers. The catalyst used for polymerization is the Ziegler–Natta catalyst, named after Karl Ziegler and Giulio Natta, who developed it in 1953. This catalyst is an organometallic complex of titanium tetrachloride and triethyl aluminum, with the active form of the catalyst being an alkyl titanium compound. Using the Ziegler–Natta...
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Fermi Level Dynamics01:12

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The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
341

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流量控制的双位基塔耶夫链.

Ivan Kulesh1, Sebastiaan L D Ten Haaf1, Qingzhen Wang1

  • 1QuTech and Kavli Institute of Nanoscience, Delft University of Technology, Delft, 2600 GA, The Netherlands.

Physical review letters
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概括
此摘要是机器生成的。

研究人员使用可调节的约瑟夫森连接在量子点中设计了Majorana绑定状态 (MBS). 通过静电和相位方法控制安德里耶夫束状态 (ABS),可以扩大MBS的参数空间,并探测它们的空间分布.

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科学领域:

  • 凝聚物质物理学 凝聚物质物理学
  • 量子信息科学是一种量子信息科学.
  • 纳米技术纳米技术

背景情况:

  • 人工基塔耶夫链在半导体-超导体混合装置中实现.
  • 安德里耶夫绑定状态 (ABS) 在这些系统中介于量子点之间的合.
  • 工程Majorana绑定状态 (MBSs) 需要精确控制ABS能量.

研究的目的:

  • 用扩展的ABS来证明使用远距离量子点之间的合的控制.
  • 调查静电和相控在扩大MBS参数空间中的作用.
  • 为了深入了解马约拉纳波函数的空间分布.

主要方法:

  • 使用可调节流量的约瑟夫森连接器来设计扩展的ABS.
  • 应用静电和相位控制机制来操纵ABS能量.
  • 在量子点之间的混合区域使用光谱探测器.

主要成果:

  • 约瑟夫森连接处的扩展ABS有效地控制了大约1微米的量子点之间的合.
  • 结合静电和相位控制可显著增加用于观察MBS的参数空间.
  • 光谱探测提供了关于马约拉纳波函数空间分布的信息.

结论:

  • 可调节流量的约瑟夫森连接点提供了一个可行的平台,可以通过ABS控制量子点合.
  • 加强对ABS的控制对于推动MBS在人工Kitaev链中的实现至关重要.
  • 这项工作提供了一种探测多站点系统中Majorana波函数定位的方法.