Related Experiment Video
Updated: Jun 5, 2025

10:02
Neutron Spin Echo Spectroscopy as a Unique Probe for Lipid Membrane Dynamics and Membrane-Protein Interactions
Published on: May 27, 2021
4.0K
Estimate of mode coupling in a spin-VECSEL
Optics Letters
|December 13, 2024
Summary
This study shows that a specific vertical-cavity surface-emitting laser (VCSEL) device prevents simultaneous dual-polarization oscillation. This characteristic, ideal for spintronic applications, results from a Lamb coupling constant near 1.
Area of Science:
- Optoelectronics
- Spintronics
- Laser Physics
Background:
- Vertical-cavity surface-emitting lasers (VCSELs) are crucial for spin injection applications.
- Understanding polarization dynamics in VCSELs is key for spintronic device development.
Purpose of the Study:
- To experimentally investigate nonlinear mode coupling between circular polarizations in a spin-injection VCSEL.
- To determine if simultaneous oscillation of both circular polarizations occurs in the studied VCSEL.
Main Methods:
- Utilized a specialized experimental setup incorporating a Faraday rotator.
- Adjusted cavity losses to control laser oscillation between left-circular and right-circular polarizations.
Main Results:
- Demonstrated that simultaneous oscillation of both left-circular and right-circular polarizations never occurs.
- The experimental results indicate a Lamb coupling constant very close to 1 for this VCSEL.
Conclusions:
- The VCSEL device exhibits strong suppression of dual-polarization oscillation.
- This property makes the device highly suitable for advanced spintronic applications requiring single polarization output.
Related Concept Videos
Spin–Spin Coupling Constant: Overview
878
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...
878
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
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
965
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...
965
Spin–Spin Coupling: One-Bond Coupling
938
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,...
938
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
¹H NMR: Long-Range Coupling
1.7K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
1.7K

