Related Experiment Video
Updated: May 24, 2025

09:00
Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
Published on: June 28, 2018
9.8K
Cavity magnon-polariton interface for strong spin-spin coupling.
Optics Letters
|February 28, 2025
Summary
Researchers propose a hybrid system for strong qubit coupling, using squeezed magnons to enhance interactions. This method enables robust, long-distance spin-spin coupling for quantum technologies.
Area of Science:
- Quantum Information Science
- Quantum Computation
- Solid-State Physics
Background:
- Strong coupling between single qubits is essential for quantum information science and computation.
- Achieving strong coupling, particularly in solid-state qubits, remains a significant challenge.
Purpose of the Study:
- To propose a novel hybrid quantum system for realizing strong long-distance spin-spin coupling.
- To leverage Kerr magnons and cavity-magnon polaritons for enhanced qubit interactions.
Main Methods:
- A hybrid system comprising a coplanar waveguide (CPW) resonator, a nitrogen-vacancy (NV) spin in diamond, and an yttrium-iron-garnet (YIG) nanosphere.
- Utilizing a strong driving field to induce the Kerr effect, squeezing magnons and exponentially enhancing resonator-magnon coupling.
- Investigating the critical phenomenon where the low-frequency polariton (LP) frequency approaches zero, leading to improved spin-LP coupling.
Main Results:
- The system generates two cavity-magnon polaritons: a high-frequency polariton (HP) and a low-frequency polariton (LP).
- At critical coupling, the NV spin decouples from the HP and strongly couples to the LP.
- Achieved strong spin-spin coupling mediated by the LP in the dispersive regime with accessible parameters.
Conclusions:
- The critical cavity-magnon polariton serves as a viable interface for strong spin-spin coupling.
- This approach offers a promising pathway for manipulating remote solid spins.
- The proposed system advances the development of robust quantum information processing.
More Related Videos
Related Concept Videos
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
939
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...
939
Spin–Spin Coupling Constant: Overview
862
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...
862
Spin–Spin Coupling: One-Bond Coupling
922
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,...
922
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
1.2K
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...
1.2K
Atomic Nuclei: Nuclear Spin State Overview
843
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of...
843

