Current Perpendicular-to-Plane (CPP) Magnetoresistance (MR)

TL;DR

This paper reviews the measurement techniques, parameters, and physical insights gained from CPP-GMR studies in multilayer structures, highlighting interface effects, spin-diffusion lengths, and device applications.

Contribution

It provides a comprehensive overview of CPP-GMR measurement methods, key parameters, and recent advances in understanding interface and bulk properties in multilayers.

Findings

Characterization of interface and bulk parameters in multilayers.

Determination of spin-diffusion lengths in ferromagnetic metals.

Progress toward CPP-MR device development.

Abstract

Measurements of Giant Magnetoresistance (GMR) in ferromagnetic/non-magnetic (F/N) multilayers with Current flow Perpendicular to the layer Planes (CPP-geometry) can give better access to the fundamental physics underlying GMR than measurements with the more usual Current flow In the layer Planes (CIP geometry). Because the same measuring current passes through all of the layers, the CPP-MR can often be described by simpler equations that allow separation of effects of scattering within the bulk of the F- and N-metals and at F/N, N1/N2, and F/S (S = superconductor) interfaces. We first describe the parameters that are used to characterize the CPP-MR, the different techniques used to measure these parameters, and the different types of multilayers used to control the two orientations of the magnetizations of adjacent F-layers, anti-parallel (AP) and parallel (P), that permit isolation of the parameters. We then detail what has been learned about the parameters of bulk F-metals, of bulk N-metals, and of F/N, N1/N2, and F/S interfaces. Especially important are the parameters of interfaces and the spin-diffusion lengths in F-metals and F-alloys, about which almost nothing was known in advance. Lastly, we describe work toward CPP-MR devices and studies of magnetothermoelectric effects, before summarizing what has been learned and listing some items not yet understood.