Abstract

The electrical properties of magnetic sensing devices fabricated from anisotropic materials are not easily extracted. Here we present a method for determining the resistance matrix for an anisotropic device with multiple electrical contacts placed in a perpendicular magnetic field. By using the methods developed by Van der Pauw and Wasscher, the analysis for the anisotropic system is reduced to the equivalent problem for an isotropic sample, which can then be solved using methods developed previously. As a result, the method works in the case of structures with an arbitrary number of asymmetric extended contacts at large magnetic field strength. In addition to the extraction of nonisotropic resistivities, the resistance matrix can be used to analyze the Hall effect for anisotropic plates.

Highlights

  • The electrical resistivity of materials is a very important property in the characterization of magnetic sensing devices

  • The electrical properties of magnetic sensing devices fabricated from anisotropic materials are not extracted

  • By using the methods developed by Van der Pauw and Wasscher, the analysis for the anisotropic system is reduced to the equivalent problem for an isotropic sample, which can be solved using methods developed previously

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Summary

Introduction

The electrical resistivity of materials is a very important property in the characterization of magnetic sensing devices. There is a large body of work devoted to the determination of the resistivity of isotropic materials dating back to the seminal work of van der Pauw [1] up through the very recent article by Oliveira, et al [2]. For the case when the voltage drop and current along one direction do not directly yield the electrical resistivity along that path, but depend on the properties in other directions as well, the material is anisotropic and its study

Homentcovschi et al DOI
The Basic Relationships for a Hall Plate with Finite Contacts
The Case of a Flat Rectangular Sample
The Case of a Circular Sample
Extraction of the Sheet Resistance
Maximizing the Hall Voltage
Conclusions

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