相关实验视频
Updated: Jul 19, 2025

10:37
Spatial Separation of Molecular Conformers and Clusters
Published on: January 9, 2014
9.0K
在Andreev分子中展示非局部约瑟夫森效应
Daniel Z Haxell1, Marco Coraiola1, Manuel Hinderling1
1IBM Research Europe-Zurich, Säumerstrasse 4, 8803 Rüschlikon, Switzerland.
Nano letters
|August 8, 2023
概括
我们展示了非局部的约瑟逊效应在合的约瑟逊连接点 (JJs),创建一个可调的φ0连接点. 这一突破使混合量子设备的新联网方案成为可能.
科学领域:
- 超导量子器件是一种超导量子器件.
- 量子信息科学是一种量子信息科学.
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 约瑟夫森连接 (JJs) 是超导电子的基础.
- 对于先进的量子技术来说,了解合的JJ中的非局部效应至关重要.
研究的目的:
- 为了研究非局部的约瑟夫森效应在合的JJs.
- 为了实现一个静电和磁性调节的 φ0 连接点.
- 为了探索安德里耶夫结合状态的杂交.
主要方法:
- 交换电流测量平面约瑟夫森交叉点.
- 独立控制超导的相位差异.
- 改变门电压和JJ之间的距离.
主要成果:
- 在JJs的电流相位关系中观察到异常相位移.
- 证明了非局部的约瑟夫森效应和可调 φ0 交叉点行为.
- 阶段转移依赖于JJ距离,与安德里耶夫束状态杂交相一致.
结论:
- 该研究实现了一个可调节的超导相源.
- 结果表明Andreev分子的形成.
- 混合量子设备中的新合方案的潜力.
相关概念视频
π Electron Effects on Chemical Shift: Overview
1.1K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.1K
Noncovalent Attractions in Biomolecules
51.9K
Noncovalent attractions are associations within and between molecules that influence the shape and structural stability of complexes. These interactions differ from covalent bonding in that they do not involve sharing of electrons.
Four types of noncovalent interactions are hydrogen bonds, van der Waals forces, ionic bonds, and hydrophobic interactions.
Hydrogen bonding results from the electrostatic attraction of a hydrogen atom covalently bonded to a strong-electronegative atom like oxygen,...
Four types of noncovalent interactions are hydrogen bonds, van der Waals forces, ionic bonds, and hydrophobic interactions.
Hydrogen bonding results from the electrostatic attraction of a hydrogen atom covalently bonded to a strong-electronegative atom like oxygen,...
51.9K
π Electron Effects on Chemical Shift: Aromatic and Antiaromatic Compounds
1.2K
In aromatic compounds, such as benzene, the circulation of (4n + 2) π-electrons sets up a diamagnetic or diatropic ring current around the perimeter of the molecule. This current induces a magnetic field that opposes the external field inside the ring and reinforces it on the outside. The protons in benzene are deshielded and exhibit high chemical shifts in the range 6.5–8.5 ppm. The shielding effect at the center of the ring is evident in complex aromatic molecules, such as...
1.2K
Inductive Effects on Chemical Shift: Overview
1.1K
The protons in unsubstituted alkanes are strongly shielded with chemical shifts below 1.8 ppm. Methine, methylene, and methyl protons appear at approximately 1.7, 1.2 and 0.7 ppm, while the proton signal from methane appears at 0.23 ppm. An electronegative substituent, such as chlorine, withdraws the electron density from the protons, increasing their chemical shift. Progressive substitution of the hydrogens in methane by chlorine shifts the proton signals increasingly downfield, to 3.05 ppm in...
1.1K
¹³C NMR: Distortionless Enhancement by Polarization Transfer (DEPT)
1.1K
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...
1.1K
Diamagnetic Shielding of Nuclei: Local Diamagnetic Current
897
An applied magnetic field causes the electrons present in the molecule to circulate, setting up a local diamagnetic current within the molecule. The local diamagnetic current arising from circulating sigma-bonding electrons induces a magnetic field, Blocal that opposes the applied magnetic field, B0. The effective magnetic field experienced by these nuclei is given by the difference between the applied and local magnetic fields in a phenomenon called local diamagnetic shielding. Essentially,...
897

