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Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

1.1K
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...
1.1K
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.1K
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,...
1.1K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.2K
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...
1.2K
Semiconductors01:22

Semiconductors

1.0K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.0K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)01:22

Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)

1.2K
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...
1.2K
Carrier Transport01:21

Carrier Transport

666
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
666

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Related Experiment Video

Updated: Oct 29, 2025

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
14:58

Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping

Published on: June 3, 2015

15.0K

Coherent spin qubit transport in silicon.

J Yoneda1,2, W Huang3,4, M Feng3

  • 1School of Electrical Engineering and Telecommunications, The University of New South Wales, Sydney, NSW, Australia. yoneda.j.aa@m.titech.ac.jp.

Nature Communications
|July 6, 2021
PubMed
Summary

Researchers achieved high-fidelity coherent transport of electron spin qubits in silicon, a crucial step for scalable quantum computing. This method enhances on-chip quantum information distribution, reducing overheads in quantum processors.

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Area of Science:

  • Quantum computing
  • Solid-state physics
  • Quantum information science

Background:

  • Scalable quantum processors require efficient qubit connectivity.
  • Current architectures with nearest-neighbor interactions incur significant qubit overheads.
  • Coherent qubit transport offers a solution for enhanced connectivity.

Purpose of the Study:

  • To demonstrate high-fidelity coherent transport of electron spin qubits.
  • To assess the impact of qubit transport on qubit fidelity.
  • To provide elements for on-chip quantum information distribution.

Main Methods:

  • Utilizing isotopically-enriched silicon for quantum dot fabrication.
  • Implementing Ramsey interferometry and quantum state tomography.
  • Observing qubit precession in the inter-site tunneling regime.

Main Results:

  • Achieved a polarization transfer fidelity of 99.97%.
  • Reported an average coherent transfer fidelity of 99.4%.
  • Demonstrated key elements for high-fidelity qubit transport.

Conclusions:

  • Coherent qubit transport in silicon is feasible with high fidelity.
  • This technique reinforces the scaling prospects of silicon-based spin qubits.
  • Enables high-fidelity, on-chip quantum information distribution.