Rashba Spin Orbit Coupling Pdf

  1. PDF Realistic Rashba and Dresselhaus spin-orbit coupling for neutral atoms.
  2. [PDF] Rashba and Weyl spin-orbit coupling in an optical lattice clock.
  3. PDF Rashba and Weyl spin-orbit coupling in an optical lattice clock.
  4. [PDF] Tuning Rashba Spin-Orbit Coupling in Gated Multilayer InSe.
  5. PDF Analogue of Rashba pseudo-spin-orbit coupling in photonic lattices by.
  6. (PDF) Effect of Rashba spin-orbit and Rabi couplings on the.
  7. (PDF) Electron pairs bound by the spin-orbit interaction in.
  8. Rashba effect - Wikipedia.
  9. Rashba spin-orbit coupling in the Kane-Mele-Hubbard model.
  10. Rashba-type spin-orbit coupling in bilayer Bose-Einstein.
  11. [PDF] Impact of the Rashba Spin Orbit Coupling on f -electron Materials.
  12. PDF Influence of Rashba spin-orbit coupling on the Kondo effect.
  13. (PDF) Effects of Rashba spin orbit coupling on the.
  14. [PDF] New perspectives for Rashba spin-orbit coupling.

PDF Realistic Rashba and Dresselhaus spin-orbit coupling for neutral atoms.

The presence of strong spin−orbit coupling (SOC) and bulk ferroelectricity in many of the (three-dimensional) 3D Rashba OMHP materials have been studied extensively.7,28−37 However, the direct role of spin and orbital degrees of freedom on photovoltaic applications are largely unexplored. An explanation of nonlinear gate voltage control of Rashba SOC can be generalized to other electrostatically gated semiconductor nanomaterials in which a similar tendency of spin-orbit length saturation was observed, and is thus of broad implications in spintronics. Manipulating the electron spin with the aid of spin-orbit coupling (SOC) is an indispensable element of spintronics.

[PDF] Rashba and Weyl spin-orbit coupling in an optical lattice clock.

SPIN-ORBIT COUPLING IN CONDENSED MATTER PHYSICS. Emmanuel I. Rashba 1 1 Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA The subject of our paper [1] with uriY A. Bychkov is two-fold spin splitting of the band spectrum of two-dimensional charge carriers, electrons and holes, in.

PDF Rashba and Weyl spin-orbit coupling in an optical lattice clock.

We report a theoretical study of the spin and valley dependent transport properties in a WSe 2 superlattice with external Rashba spin-orbit interaction (ERSOI). It is shown that the conductance with and without spin flip strongly depends on the ERSOI and has an oscillatory behavior with respect to ERSOI strength, thus WSe 2 superlattice can act as a spin-converter.

[PDF] Tuning Rashba Spin-Orbit Coupling in Gated Multilayer InSe.

(Extrinsic) Spin-Hall Effect Spin Hall Effect: the regular current (J) drives a spin current (J s) across the bar resulting in a spin accumulation at the edges. F SO J F SO J s More spin up electrons are deflected to the right than to the left (and viceversa for spin down) For a given deflection, spin up and spin down electrons make a side.

PDF Analogue of Rashba pseudo-spin-orbit coupling in photonic lattices by.

Lar and spin-orbit (SO) coupled BECs, etc. [4–14]. In this paper we investigate the effect of the Rabi and Rash ba spin-orbit coupling on the dynamical stability of the bi- nary BEC system. In BECs,. While these aspects of organometal halide perovskites have attracted the most attention, the consequences of the Rashba effect, driven by strong spin-orbit coupling, on the photovoltaic properties.

(PDF) Effect of Rashba spin-orbit and Rabi couplings on the.

PDF | We show that the bound electron pairs (BEPs) emerge in two-dimensional gated Rashba materials owing to the interplay of the pair spin-orbit... | Find, read and cite all the research you need.

(PDF) Electron pairs bound by the spin-orbit interaction in.

Manipulating the electron spin with the aid of spin-orbit coupling (SOC) is an indispensable element of spintronics. Electrostatically gating a material with strong SOC results in an effective magnetic field which can in turn be used to govern the electron spin. In this work, we report the existence and electrostatic tunability of Rashba SOC in multilayer InSe. We observed a gate-voltage-tuned. The Rashba spin–orbit cou- pling produces spin flipping in the conductivity. The spin flipping occurs at sharp resonance peaks. This sharp anomaly at the edges of the conductance plateaus is behind the sudden increase of the spin-flip phenomenon.43,44 BY increasing the Fig. 3.

Rashba effect - Wikipedia.

The Plasma Oscillations in a Two-Dimensional Electron-Hole Liquid Under Influence Rashba Spin-Orbit Coupling. Journal of Nanoelectronics and Optoelectronics, 2013. Michael A Liberman. Download Download PDF. Full PDF Package Download Full PDF Package. PHYSICAL REVIEW A 84, 025602 (2011) Realistic Rashba and Dresselhaus spin-orbit coupling for neutral atoms D. L. Campbell,1 G. Juzeliunas,¯ 2 and I. B. Spielman1 1Joint Quantum Institute, National Institute of Standards and Technology, and University of Maryland, Gaithersburg, Maryland 20899, USA 2Institute of Theoretical Physics and Astronomy, Vilnius University, A.

Rashba spin-orbit coupling in the Kane-Mele-Hubbard model.

This Review discusses relevant recent and ongoing realizations of Rashba physics in condensed matter, ranging from layered graphene-like materials to cold atoms. In 1984, Bychkov and Rashba introduced a simple form of spin-orbit coupling to explain the peculiarities of electron spin resonance in two-dimensional semiconductors. Over the past 30 years, Rashba spin-orbit coupling has inspired a. Recent experimental realization of one-dimensional (1D) spin-orbit coupling (SOC) for ultracold alkaline-earth(-like) atoms in optical lattice clocks opens a new avenue for exploring exotic quantum matter because of the strongly suppressed heating of atoms from lasers comparing with alkaline atoms. Here we propose a scheme to realize two-dimensional (2D) Rashba and three-dimensional (3D) Weyl.

Rashba-type spin-orbit coupling in bilayer Bose-Einstein.

In 1984, Bychkov and Rashba introduced a simple form of spin–orbit coupling to explain the peculiarities of electron spin reso- nance in two-dimensional semiconductors. The Rashba spin-orbit coupling is typical for systems with uniaxial symmetry, e.g., for hexagonal crystals of CdS and CdSe for which it was originally found and perovskites, and also for heterostructures where it develops as a result of a symmetry breaking field in the direction perpendicular to the 2D surface.

[PDF] Impact of the Rashba Spin Orbit Coupling on f -electron Materials.

The Rashba spin-orbit coupling coefficient in silicon quantum wells and find theT1 and T2 times of the spins from this mechanism as a function of momentum scattering time, magnetic field, and device-specific param-eters. We obtain agreement with existing data for the angular dependence of the relaxation times and show that. Results are summarized in Fig. 1. For small Rashba coupling, we find the TI (at small onsite interaction U) and XY-AFM phases (at large interactions U) which are also present in the Kane-Mele-Hubbard model without the Rashba coupling. Larger Rashba coupling induces a topologically nontrivial direct-gap-only semiconductor before the system..

PDF Influence of Rashba spin-orbit coupling on the Kondo effect.

For the linear Rashba SO coupling of the semiconductor conduction band can reproduce the behavior of more sophisticated eight-band k ·p model calculations. This is achieved by adjusting a single effective parameter that depends on the nanowire crystal structure and its chemical composition. We further compare our results to the. The combination of strong spin orbit coupling and strong correlations holds tremendous potential for interesting physical phenomena as well as applications in spintronics and quantum computation. In this context, we here study the interplay between the Rashba spin-orbit coupling (RSOC) and the Kondo screening in noncentrosymmetric f -electron materials. We show that the Kondo coupling of the f.

(PDF) Effects of Rashba spin orbit coupling on the.

Idea of manipulating spin states to create new, spin-based electronic devices [1,2]. Rashba spin-orbit (SO) coupling [3] has been proposed as a mechanism for spin control, not only because of the possibility of its external manipulation, but also because it is the physical origin of spin-dependent phenomena such as anisotropic magnetoresistance.

[PDF] New perspectives for Rashba spin-orbit coupling.

Of the electron spin transistor have also been suggested [6,7]. An important ingredient of the DDT is the spin-orbit coupling of the Rashba [8–10] or Dresselhaus [11,12] types. This Rashba-Dresselhaus (RD) coupling scheme is described by a vector potential which can be made proportional to the spin-1/2 operator of a particle within a plane.


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