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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
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A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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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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A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
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A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
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  1. 首页
  2. 高相干超导量子比特的重叠连接点.
  1. 首页
  2. 高相干超导量子比特的重叠连接点.

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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高相干超导量子比特的重叠连接点.

X Wu1, J L Long1,2, H S Ku1

  • 1National Institute of Standards and Technology, Boulder, Colorado 80305, USA.

Applied physics letters
|March 12, 2025

在PubMed 上查看摘要

概括
此摘要是机器生成的。

研究人员使用in situ Ar削制造了用于超导量子的亚微米约瑟夫森连接点. 这种清洗方法提高了连贯性,简化了制造,为改进量子比特制造铺平了道路.

关键词:
03.67.Lxx 在 03.67.Lx 在

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科学领域:

  • 量子计算是一种量子计算.
  • 超导电子产品的超导电子
  • 材料科学 是一种材料科学.

背景情况:

  • 高相干超导量子比特对于量子计算至关重要.
  • 制造具有高产量和连贯性的亚微米约瑟夫森连接仍然是一个挑战.
  • 现有的方法通常依赖于取决于角度的阴影面罩,限制了可扩展性.

研究的目的:

  • 用标准加工技术演示制造亚微米约瑟夫森连接器的方法.
  • 为了研究现场Ar削对表面的影响,以形成接口.
  • 为了在超导量子比特的约瑟夫森交叉点中实现高连贯性.

主要方法:

  • 采用了两步 lithography 和正常角度蒸发.
  • 在氧化之前在现场采用 (Ar) 磨来清洁表面.
  • 使用电子束光刻和添加过程定义了顶部和底部电极.

主要成果:

  • 成功制造了微米以下的约瑟夫森连接器.
  • 在Ar磨表面形成的连接处实现了高连贯性.
  • 消除了依赖角度的阴影面具的需要,简化了这个过程.
  • 与传统的CMOS处理证明兼容,可提高利率和产量.

结论:

  • 在表面的现场研磨是制造高连贯性约瑟夫森连接的可行方法.
  • 这种技术简化了制造,有利于超导量子比特的可扩展制造.
  • 展示的方法支持将先进的量子比特制造与标准半导体处理集成在一起.