Abstract

High-conductive phosphorus-doped Si nanocrystals/SiO2(nc-Si/SiO2) multilayers are obtained, and the formation of Si nanocrystals with the average crystal size of 6 nm is confirmed by high-resolution transmission electron microscopy and Raman spectra. The temperature-dependent carrier transport behaviors of the nc-Si/SiO2 films are systematically studied by which we find the shift of Fermi level on account of the changing P doping concentration. By controlling the P doping concentration in the films, the room temperature conductivity can be enhanced by seven orders of magnitude than the un-doped sample, reaching values up to 110 S/cm for heavily doped sample. The changes from Mott variable-range hopping process to thermally activation conduction process with the temperature are identified and discussed.

Highlights

  • Nanocrystalline Si materials have been extensively studied because of their novel properties and their potential applications in future electronic and optoelectronic devices [1, 2]

  • We found that the conductivity data of the doped Nanocrystalline Si (nc-Si)/SiO2 multilayers obtained below the room temperature (300 K) cannot be well described by the Arrhenius relationship which suggests different mechanisms dominating the carrier transport processes

  • In summary, un-doped and P-doped nc-Si/SiO2 multilayers are formed by 1000 °C thermal annealing the corresponding hydrogenated amorphous Si/SiO2 stacked structures

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Summary

Introduction

Nanocrystalline Si (nc-Si) materials have been extensively studied because of their novel properties and their potential applications in future electronic and optoelectronic devices [1, 2]. It has been reported that nc-Si-based materials can be potentially used in light-emitting devices as well as generation solar cells [4,5,6]. Most of the published work focused on the un-doped nc-Si materials. In order to further improve the devices performance, it is necessary to study the doping effect in nc-Si materials, since it can effectively control the electronic structures and properties of semiconductors [7, 8]. It was reported that the doping of P and B in nc-Si is difficult due to Self-Purification effect, which is quite different from their bulk counterpart [8,9,10].

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