Abstract

Spintronics, which manipulate spins but not electron charge, are highly valued as energy and thermal dissipationless systems. A variety of materials are challenging the realization of spintronic devices. Among those, graphene, a carbon mono-atomic layer, is very promising for efficient spin manipulation and the creation of a full spectrum of beyond-CMOS spin-based nano-devices. In the present article, the recent advancements in graphene spintronics are reviewed, introducing the observation of spin coherence and the spin Hall effect. Some research has reported the strong spin coherence of graphene. Avoiding undesirable influences from the substrate are crucial. Magnetism and spintronics arising from graphene edges are reviewed based on my previous results. In spite of carbon-based material with only sp2 bonds, the zigzag-type atomic structure of graphene edges theoretically produces spontaneous spin polarization of electrons due to mutual Coulomb interaction of extremely high electron density of states (edge states) localizing at the flat energy band. We fabricate honeycomb-like arrays of low-defect hexagonal nanopores (graphene nanomeshes; GNMs) on graphenes, which produce a large amount of zigzag pore edges, by using a nonlithographic method (nanoporous alumina templates) and critical temperature annealing under high vacuum and hydrogen atmosphere. We observe large-magnitude ferromagnetism, which arises from polarized spins localizing at the hydrogen-terminated zigzag-nanopore edges of the GNMs, even at room temperature. Moreover, spin pumping effects are found for magnetic fields applied in parallel with the few-layer GNM planes. Strong spin coherence and spontaneously polarized edge spins of graphene can be expected to lead to novel spintronics with invisible, flexible, and ultra-light (wearable) features.

Highlights

  • Spintronics are highly promising as a key technology for generation [1–7]

  • We fabricate honeycomb-like arrays of low-defect hexagonal nanopores on graphenes, which produce a large amount of zigzag pore edges, by using a nonlithographic method and critical temperature annealing under high vacuum and hydrogen atmosphere

  • In [30,31], it is suggested that the zigzag edge is the most stable chemically and that arm chair-based edges are reconstructed to zigzag after STM Joule heating for long edges of overlapped graphenes [30] and electron beam (EB) irradiation for pore edges [31]

Read more

Summary

Introduction

Spintronics are highly promising as a key technology for generation [1–7]. They have the following two prospects: (1) Zero-emission energy and (2) replacement of CMOS technology (i.e., beyond CMOS). One is the graphene nanoribbon (GNR) model, which assumes perfect edge atomic structures without any defects It allows that the electron spins localizing at zigzag edges [18] to become stabilized toward polarization (i.e., (anti)ferromagnetism) due to the exchange interaction between the two edges. The presence of low-concentration defects in ensemble of carbon atoms (e.g., graphene flakes) results in the appearance of net magnetism It predicts the emergence of ferromagnetism by an increase in the difference between the number of removed A and B sites (∆AB) of the graphene bipartite lattice at zigzag edges [39,41].

Spin Coherence in Graphene
Spin Hall Effect
Magnetism and Spintronics on Pore Edge Spins in Graphene Nanomeshes
Sample Fabrication for GNMs
Magnetism on Pore Edge Termination by Different Foreign Atoms
Theoretical Confirmation by Two Models
Spin-Based Phenomena in MR Measurements of Few-Layer GNMs
Findings
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call