在 Josephson 交叉点附近的 P 波配对
Rubén Seoane Souto1, Dushko Kuzmanovski2, Ignacio Sardinero3,4,5
1Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC), Sor Juana Inés de la Cruz 3, 28049 Madrid, Spain.
概括
在自旋分裂超导体中,约瑟夫森交点表现出由于安德里耶夫绑定状态而导致的基态过渡. 这种过渡抑制了超电流,表明向p波配对的转变.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子材料是一种量子材料.
背景情况:
- 超导和磁性是相互竞争的现象,可以共存,导致新的量子行为.
- 它们的相互作用可以诱导异国情调的电子配对机制和拓相.
研究的目的:
- 研究由两个自旋分裂超导体形成的约瑟夫森结的特性.
- 了解安德里耶夫结态在结点行为中的作用.
主要方法:
- 约瑟夫森连接与自旋分裂超导体的理论研究.
- 分析安德里耶夫结合状态及其能量水平.
- 检查配对通道和噪声频谱.
主要成果:
- 一个基态过渡发生在一个Andreev绑定状态穿过费米水平时,导致压抑的超电流.
- 这种超级电流封锁归因于p波对接在接口附近的主导地位.
- 通过并行磁化,P波配对得到了青,而通过反并行磁化则被抑制.
- 噪声频谱透露了通过升高的零频噪声通过基态过渡的信号.
结论:
- 这项研究揭示了自旋分裂超导体约瑟夫森连接处的新型基态过渡.
- 这些发现凸显了p波配对在这些系统中的重要性.
- 结果为控制和理解混合超导体系统中的奇异量子现象提供了洞察力.
相关概念视频
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
977
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...
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...
977
Spin–Spin Coupling Constant: Overview
891
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...
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...
891
Spin–Spin Coupling: One-Bond Coupling
949
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,...
949
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)
1.0K
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...
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...
1.0K
NMR Spectroscopy: Spin–Spin Coupling
1.3K
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
¹H NMR Signal Multiplicity: Splitting Patterns
5.0K
When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
5.0K


