Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)01:20

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

1.1K
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...
1.1K
Spin–Spin Coupling Constant: Overview01:08

Spin–Spin Coupling Constant: Overview

961
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...
961
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

284
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
284
Raman Spectroscopy: Overview01:20

Raman Spectroscopy: Overview

472
The underlying principle of Raman spectroscopy is based on the interaction between light and matter, specifically molecules' inelastic scattering of photons. When a monochromatic beam of light, typically from a laser source, interacts with a sample, most scattered light has the same frequency as the incident light. This is known as Rayleigh scattering.
However, a small fraction of the scattered light exhibits a frequency shift due to the exchange of energy between the incident photons and...
472
Spin–Spin Coupling: One-Bond Coupling01:17

Spin–Spin Coupling: One-Bond Coupling

1.0K
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,...
1.0K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

8.9K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
8.9K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

APASA: adaptive selection of informative peritumoral regions for improved automated cancer lesion analysis.

Scientific reports·2026
Same author

Flatband Resonance Enhanced Second-Harmonic Generation in Thin-Film Lithium Niobate Moiré Microcavity.

Nano letters·2026
Same author

Conformational bifurcation drives dual transport regimes in molecular junctions: Unsupervised machine learning insights.

Smart molecules : open access·2026
Same author

An optically controlled synaptic device based on a PdSe<sub>2</sub>/α-In<sub>2</sub>Se<sub>3</sub> vdW heterostructure FET.

Materials horizons·2026
Same author

A Temperature-Pressure Dual-Mode Flexible Patch Sensor with Temperature Compensation and Pressure Decoupling Functions for Pulse Detection and Recognition.

ACS sensors·2026
Same author

Quantitative and Visual Detection of Pseudouridine at Specific Sites Using Bisulfite-Assisted Rolling Circle Amplification.

Analytical chemistry·2026
Same journal

A highly conductive polar metal with efficient charge-spin conversion.

Nature materials·2026
Same journal

Giant and broadband circular dichroism from particle-hole symmetry breaking in Weyl semimetals.

Nature materials·2026
Same journal

Lattice distortion activates deformation twinning in ultrastrong steel.

Nature materials·2026
Same journal

Methane storage using metal-dipyrazolate frameworks.

Nature materials·2026
Same journal

Nanotechnology-mediated precision delivery of mRNA.

Nature materials·2026
Same journal

Operando microscopy for neuromorphic hardware.

Nature materials·2026
See all related articles
  1. Home
  2. Spin-valley Rashba Monolayer Laser.
  1. Home
  2. Spin-valley Rashba Monolayer Laser.

Related Experiment Video

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.0K

Spin-valley Rashba monolayer laser.

Kexiu Rong1, Xiaoyang Duan1, Bo Wang2

  • 1Atomic-Scale Photonics Laboratory, Russell Berrie Nanotechnology Institute, and Helen Diller Quantum Center, Technion - Israel Institute of Technology, Haifa, Israel.

Nature Materials
|July 6, 2023

View abstract on PubMed

Summary
This summary is machine-generated.

Researchers developed a novel spin-optical laser using a tungsten disulfide (WS₂) monolayer. This atomic-scale light source demonstrates robust spin polarization and coherence at room temperature, paving the way for advanced optical technologies.

More Related Videos

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
12:21

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators

Published on: April 4, 2016

11.3K
Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

12.9K

Related Experiment Videos

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser
09:00

Experimental Methods for Spin- and Angle-Resolved Photoemission Spectroscopy Combined with Polarization-Variable Laser

Published on: June 28, 2018

10.0K
Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators
12:21

Stimulated Stokes and Antistokes Raman Scattering in Microspherical Whispering Gallery Mode Resonators

Published on: April 4, 2016

11.3K
Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

12.9K

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Optoelectronics

Background:

  • Direct-bandgap transition metal dichalcogenide monolayers exhibit valley-contrasting optical selection rules, making them promising for spin-optical applications.
  • Atomic-scale light sources are crucial for next-generation optoelectronic devices.

Purpose of the Study:

  • To demonstrate a spin-optical monolayer laser utilizing a WS₂ monolayer integrated into a microcavity.
  • To investigate the generation and properties of photonic spin-valley resonances.

Main Methods:

  • Incorporation of a WS₂ monolayer into a heterostructure microcavity.
  • Generation of spin-valley modes via photonic Rashba-type spin splitting of a bound state in the continuum.
  • Utilizing inversion symmetry breaking to induce photonic spin-orbit interaction.

Main Results:

  • Demonstration of a functional spin-optical monolayer laser with intrinsic spin polarizations.
  • Observation of high spatial and temporal coherence in the laser output.
  • Achieved valley coherence in the WS₂ monolayer under arbitrary pump polarizations at room temperature.
  • Exhibited symmetry-enabled robustness features.

Conclusions:

  • The developed monolayer laser integrates electron and photon spins for coherent light generation.
  • Monolayer-integrated spin-valley microcavities offer new possibilities for classical and non-classical spin-optical light sources.
  • This work advances the development of atomic-scale, coherent spin-optical devices.