Abstract

Fabrication processes of thin boron-doped nanocrystalline diamond (B-NCD) films on silicon-based micro- and nano-electromechanical structures have been investigated. B-NCD films were deposited using microwave plasma assisted chemical vapour deposition method. The variation in B-NCD morphology, structure and optical parameters was particularly investigated. The use of truncated cone-shaped substrate holder enabled to grow thin fully encapsulated nanocrystalline diamond film with a thickness of approx. 60 nm and RMS roughness of 17 nm. Raman spectra present the typical boron-doped nanocrystalline diamond line recorded at 1148 cm−1. Moreover, the change in mechanical parameters of silicon cantilevers over-coated with boron-doped diamond films was investigated with laser vibrometer. The increase of resonance to frequency of over-coated cantilever is attributed to the change in spring constant caused by B-NCD coating. Topography and electrical parameters of boron-doped diamond films were investigated by tapping mode AFM and electrical mode of AFM–Kelvin probe force microscopy (KPFM). The crystallite–grain size was recorded at 153 and 238 nm for boron-doped film and undoped, respectively. Based on the contact potential difference data from the KPFM measurements, the work function of diamond layers was estimated. For the undoped diamond films, average CPD of 650 mV and for boron-doped layer 155 mV were achieved. Based on CPD values, the values of work functions were calculated as 4.65 and 5.15 eV for doped and undoped diamond film, respectively. Boron doping increases the carrier density and the conductivity of the material and, consequently, the Fermi level.

Highlights

  • Micro-electromechanical systems (MEMS) and nanoelectromechanical systems (NEMS) provide ample sensing opportunities [1]

  • The B-NCD results in high conductivity coverage of cantilever with surface resistivity of 30 m X cm and typical boron-doped nanocrystalline diamond line at 1148 cm-1 recorded by Raman spectroscopy

  • The atomic force microscope (AFM) topography showed that crystallite–grain size was 153 nm and 238 nm for boron-doped film and undoped, respectively

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Summary

Introduction

Micro-electromechanical systems (MEMS) and nanoelectromechanical systems (NEMS) provide ample sensing opportunities [1]. For characterization of surface properties at the nanoscale, atomic force microscope (AFM) has been widely used [2,3,4,5]. Since the AFM and its applications are based on the interaction between an extremely sharp probe and the sample, the probe surface is one of the crucial concerns. Characterization at the nanoscale based on the electrical conductivity and the absence of an electronic surface barrier is beneficial. Scanning tunnelling microscopy (STM) and conductive atomic force microscopy (C-AFM) with locally performed C-AFM current– voltage measurements and Kelvin probe force microscopy (KPFM) are the most effective surface analysis methods [6,7,8] with atomic- or nanometre-scale spatial resolution requiring high conductivity probes

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