Abstract

Single crystalline tungsten nanowires were prepared from directionally solidified NiAl‐W alloys by a chemical release from the resulting binary phase material. Electron back scatter diffraction (EBSD) proves that they are single crystals having identical crystallographic orientation. Mechanical investigations such as bending tests, lateral force measurements, and mechanical resonance measurements were performed on 100–300 nm diameter wires. The wires could be either directly employed using micro tweezers, as a singly clamped nanowire or in a doubly clamped nanobridge. The mechanical tests exhibit a surprisingly high flexibility for such a brittle material resulting from the small dimensions. Force displacement measurements on singly clamped W nanowires by an AFM measurement allowed the determination of a Young′s modulus of 332 GPa very close to the bulk value of 355 GPa. Doubly clamped W nanowires were employed as resonant oscillating nanowires in a magnetomotively driven resonator running at 117 kHz. The Young′s modulus determined from this setup was found to be higher 450 GPa which is likely to be an artefact resulting from the shift of the resonance frequency by an additional mass loading.

Highlights

  • Tungsten is a brittle refractory metal that crystallises in the BCC form [1]

  • None of the techniques is able to yield a self-organised array of the single crystalline tungsten nanowires except the method presented here

  • The patterns obtained from different nanowires show welldefined Kikuchi lines, proving that they are single crystalline

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Summary

INTRODUCTION

Tungsten is a brittle refractory metal that crystallises in the BCC form [1] It has high-tensile strength and good creep resistance. The dislocations will accumulate at the nanowires surface generating virtually dislocation free structures These structures exhibit mechanical strength that may reach the theoretical limit. This is especially true if the wires are single crystalline [7]. By controlling the growth parameters and the dissolution conditions, the diameter [16] and the released length [15, 17], respectively, are well adjustable The advantage of this system is that an array of nanowires is produced which allows studying the anisotropy of the mechanical properties. The influence of the contamination and oxidation in air on the elastic behaviour is studied qualitatively in static bending experiments as well as in resonant oscillating nanomechanical devices

Preparation of the nanowires
Nanowire release
Preparation of nanowires for mechanical investigation
Chemical and structural characterisation
Mechanical characterisation
Analysis of resonant oscillating nanowires
Nanowire crystallography
Flexibility
Young’s modulus of nanowires by static bending
Young’s modulus from resonant oscillating nanowires
SUMMARY
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