Related Experiment Video
Updated: Feb 12, 2026

06:53
Author Spotlight: Enhancing CryoEM Resolution Using Graphene-Coated Grids
Published on: September 8, 2023
4.0K
Strong Anisotropic Spin-Orbit Interaction Induced in Graphene by Monolayer WS_{2}
T Wakamura1, F Reale2, P Palczynski2
1Laboratoire de Physique des Solides, Université Paris-Sud, 91400 Orsay, France.
Physical Review Letters
|March 24, 2018
Summary
Monolayer transition metal dichalcogenide induces strong spin-orbit interaction (SOI) in graphene, significantly stronger than bulk materials. This finding opens new avenues for spintronic device applications.
Area of Science:
- Condensed matter physics
- Materials science
- Spintronics
Background:
- Spin-orbit interaction (SOI) is crucial for spintronics.
- Graphene's potential for spintronic applications is hindered by weak intrinsic SOI.
- Transition metal dichalcogenides (TMDs) are known to possess strong SOI.
Purpose of the Study:
- To investigate the induction of anisotropic SOI in graphene by monolayer tungsten disulfide (WS2).
- To compare the SOI induced by monolayer WS2 versus bulk WS2 in graphene.
- To determine the characteristics and magnitude of the induced SOI.
Main Methods:
- Fabrication of graphene-monolayer WS2 and graphene-bulk WS2 heterostructures.
- Magnetotransport measurements to probe spin-orbit effects.
- Theoretical analysis of weak antilocalization (WAL) curves.
Main Results:
- Monolayer WS2 induces significantly stronger anisotropic SOI in graphene than bulk WS2.
- Estimated spin-orbit energy (E_so) exceeds 10 meV.
- Experimental data is best explained by a dominant z→-z symmetric SOI and Kane-Mele SOI.
Conclusions:
- Monolayer TMDs are highly effective in inducing strong SOI in graphene.
- The findings suggest potential for novel spintronic devices utilizing graphene-TMD heterostructures.
- Elliot-Yafet mechanism and Kane-Mele SOI contribute to spin relaxation and transport properties.
More Related Videos
Related Concept Videos
Electron Orbital Model
72.9K
Orbitals are the areas outside of the atomic nucleus where electrons are most likely to reside. They are characterized by different energy levels, shapes, and three-dimensional orientations. The location of electrons is described most generally by a shell or principal energy level, then by a subshell within each shell, and finally, by individual orbitals found within the subshells.
The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
72.9K
Titration Calculations: Strong Acid - Strong Base
34.1K
Calculating pH for Titration Solutions: Strong Acid/Strong Base
A titration is carried out for 25.00 mL of 0.100 M HCl (strong acid) with 0.100 M of a strong base NaOH. The pH at different volumes of added base solution can be calculated as follows:
(a) Titrant volume = 0 mL. The solution pH is due to the acid ionization of HCl. Because this is a strong acid, the ionization is complete and the hydronium ion molarity is 0.100 M. The pH of the solution is then:
A titration is carried out for 25.00 mL of 0.100 M HCl (strong acid) with 0.100 M of a strong base NaOH. The pH at different volumes of added base solution can be calculated as follows:
(a) Titrant volume = 0 mL. The solution pH is due to the acid ionization of HCl. Because this is a strong acid, the ionization is complete and the hydronium ion molarity is 0.100 M. The pH of the solution is then:
34.1K
Molecular Orbital Theory I
47.8K
Overview of Molecular Orbital Theory
47.8K
The Energies of Atomic Orbitals
30.3K
In an atom, the negatively charged electrons are attracted to the positively charged nucleus. In a multielectron atom, electron-electron repulsions are also observed. The attractive and repulsive forces are dependent on the distance between the particles, as well as the sign and magnitude of the charges on the individual particles. When the charges on the particles are opposite, they attract each other. If both particles have the same charge, they repel each other.
30.3K
Atomic Orbitals
45.2K
An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
45.2K
Molecular Orbital Theory II
27.7K
Molecular Orbital Energy Diagrams
27.7K

