Abstract

We discuss how the emission of electrons and ions during electron-beam-induced physical vapor deposition can cause problems in micro- and nanofabrication processes. After giving a short overview of different types of radiation emitted from an electron-beam (e-beam) evaporator and how the amount of radiation depends on different deposition parameters and conditions, we highlight two phenomena in more detail: First, we discuss an unintentional shadow evaporation beneath the undercut of a resist layer caused by the one part of the metal vapor which got ionized by electron-impact ionization. These ions first lead to an unintentional build-up of charges on the sample, which in turn results in an electrostatic deflection of subsequently incoming ionized metal atoms toward the undercut of the resist. Second, we show how low-energy secondary electrons during the metallization process can cause cross-linking, blisters, and bubbles in the respective resist layer used for defining micro- and nanostructures in an e-beam lithography process. After the metal deposition, the cross-linked resist may lead to significant problems in the lift-off process and causes leftover residues on the device. We provide a troubleshooting guide on how to minimize these effects, which e.g. includes the correct alignment of the e-beam, the avoidance of contaminations in the crucible and, most importantly, the installation of deflector electrodes within the evaporation chamber.

Highlights

  • Electron-beam-induced physical vapor deposition (e-beam deposition) has developed into a versatile tool in the field of micro- and nanofabrication:[1,2,3] Compared to resistive evaporation techniques, e-beam deposition allows the evaporation of a larger variety of materials, including many oxides and metals with very low vapor pressures

  • After giving a short overview of different types of radiation emitted from an electron-beam (e-beam) evaporator and how the amount of radiation depends on different deposition parameters and conditions, we highlight two phenomena in more detail: First, we discuss an unintentional shadow evaporation beneath the undercut of a resist layer caused by the one part of the metal vapor which got ionized by electron-impact ionization

  • In this article we first give an overview on different types of radiation that are emitted during e-beam evaporation and how the amount of radiation depends on different deposition parameters and conditions

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Summary

INTRODUCTION

Electron-beam-induced physical vapor deposition (e-beam deposition) has developed into a versatile tool in the field of micro- and nanofabrication:[1,2,3] Compared to resistive evaporation techniques, e-beam deposition allows the evaporation of a larger variety of materials, including many oxides and metals with very low vapor pressures. There are drawbacks in using e-beam deposition, which include the generation of X-rays, the emission of electrons over a large energy range, and the creation of ions by electron-impact ionization, which all can lead to problems in device fabrication.[1,2,3] Especially in the field of semiconductor technology, it is well documented that radiation emitted by an e-beam evaporator can induce defects in the semiconductor material.[4,5,6,7,8] Possible side-effects of e-beam evaporation on other aspects of micro- and nanofabrication, e.g., lift-off problems of resist defined patterns,[9,10] are far less reported.

Partially ionized vapor
Secondary and backscattered electrons
Electromagnetic radiation
SHADOW DEPOSITION DUE TO IONIZED METAL VAPOR
DAMAGE OF RESIST LAYER AND LIFT-OFF PROBLEMS CAUSED BY ELECTRONS
TROUBLESHOOTING
Workarounds to diminish the problems
Identifying contaminations of evaporation material
Sources of contamination
Estimating resist temperature during deposition
Reducing electron exposure to the sample
CONCLUSION
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